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The European Solar Physics Meetings (ESPM) are organised every three years by the board of the European Solar Physics Division (ESPD), a joint division of the European Physical Society (EPS) and the European Astronomical Society (EAS). The meetings bring together a large number of from Europe and beyond, who are active in the theoretical and observational study of solar phenomena.
The 16th European Solar Physics Meeting (ESPM-16), originally planned for 2020, took place as a virtual online meeting in 6-10 September 2021, with free registration for all participants.
You can access the posters and presentation materials uploaded by the authors in the meeting timetable.
In global dynamo models, the process of magnetic flux emergence through the stellar convection zone is thought to be crucial. In the Sun, it is the strong toroidal structures built at the base of the convection zone which are assumed to be unstable to a buoyancy instability and rise through the convection zone to produce sunspots. The details of how these buoyant structures are formed, evolve and interact inside the convection zone and emerge at the photosphere and beyond are still a matter of active research. Moreover, the ability of these emergence processes to take part into the whole dynamo process is also a matter of intense debate in the solar dynamo community.
We propose in this talk to review some aspects of magnetic flux emergence in the Sun and to connect those studies with the global picture of the solar dynamo mechanism.
Mean-field dynamo theory is a rich field that tries to reproduce and often predict the large-scale behavior of a turbulent system. Numerical simulations play the same role as astronomical observations, except that the former ones can be done under controlled conditions while the latter ones have the advantage of being more in the asymptotic regime of large magnetic and fluid Reynolds numbers. Unfortunately, we do not yet understand much about the turbulence in the real Sun. Especially the extreme stratification in the uppermost layers is impossible to simulate properly.
Three-dimensional numerical simulations of the Sun are still far from the actual Sun, but they do produce features that are in agreement with appropriately tailored mean-field calculations. This has been achieved by measuring their mean-field transport coefficients using the test-field method, a reliable procedure whose accuracy enables us to pinpoint some previously unexpected phenomena.
Additional diagnostics concerning the measurement of magnetic helicity both at the solar surface and in the solar wind have widened the horizon of our understanding. In particular, it is now possible to solve mean-field models that encompass both dynamo and its wind emanating from it. In my talk, I will connect various aspects of solar wind physics with related aspects of solar magnetic activity. Looking around at other stars helps us further to put the Sun and our models into context and to appreciate to what extent our Sun might be special.
What sets the 11-year period of the solar activity cycle? Why do sunspots appear in the butterfly wings which propagate equatorward over the course of a cycle? The Babcock-Leighton flux-transport model attempts to answer these questions but has free paramters. Some of these free parameters have recently been observationally constrained. In particular, the meridional flow has recently been determined by Gizon et al. and the toroidal flux loss through the solar surface has been shown to remove most of the flux produced by the Omega effect. We show that the Babcock-Leigton FTD model can produce solar like solutions with these new constraints. We also show that the remaining parameters (mainly radial magnetic pumping and turbulent diffusivity) can produce butterfly diagrams similar to the Sun’s without artificial restrictions of the emergence latitude. The basic mechanism here is that the toroidal field is quickly transported to the bottom half of the convection zone where the meridional flow is equatorward. Thus the Babcock-Leighton FTD model remains an extremely promising candidate for how the Sun’s dynamo actually works.
The results of helioseismological inferences of subsurface flow velocities by time–distance techniques are used to analyse the spatial structure of subphotospheric convection. The source data are obtained from the Helioseismic and Magnetic Imager onboard the Solar Dynamics Observatory from May 2010 to September 2020. The helioseismic-inversion results produce the three-dimensional flow fields in a 19-Mm deep layer below the photosphere in a range of latitudes and Stonyhurst longitudes from − 60° to + 60° with an 8-hour cadence. We study the convective flow structures of various scales and shapes by applying a spherical harmonic transform to the horizontal-velocity-divergence field. The results reveal a signature of large-scale flow cells in the spatial power spectrum, which may represent the “giant cells” of solar convection. In particular, indications are found for meridionally elongated flow cells, which are considerably smaller in the longitudinal direction than in latitude. The physical properties of the multi-scale convection cells and their evolution in the course of the solar activity cycle are discussed.
The rotation rates of solar active and ephemeral regions depend on morphology and size of magnetic structures, although the reasons of the dependence are still being discussed. The aim of the work is to analyze the rotation rates of different types of magnetic tracers using magnetic field data rather than white-light images.
Magnetic field maps provided by the Helioseismic and Magnetic Imager on board the Solar Dynamics Observatory were used to measure the rotation rates of 864 active and 322 ephemeral regions observed between 2010 and 2016. We found smaller magnetic tracers to show a tendency to rotate faster as compared to larger ones. Thus, ephemeral regions exhibit on average the fastest rotation rate. We further divided active regions into three classes. Class A comprised magnetic bipoles obeying Hale’s polarity law and Joy’s law. The second class B included active regions violating at least one of these laws. The third class U comprised unipolar active regions.
We found no significant difference between the rotation rates of active regions of classes A and B. In contrast, unipolar active regions exhibited lower rotation rate and narrower distribution of the rotation rate differences. Assuming the rotation rate to indicate the anchoring depth of the magnetic structure within the convection zone, we supposed that active regions of classes A and B might be anchored throughout the entire convective envelope while unipolar active regions are rooted within a thin layer located either near the base of the convection zone or at a shallow near-surface depth.
We use SOHO and SDO data to study 2046 active regions (ARs) of the 23rd and 1507 ARs of the 24th solar cycles. According to empiric regularities for sunspot groups (Hale’s polarity law, Joy’s law, etc.) and the magneto-morphological classification (MMC), all ARs were divided into three types: A-type – regular bipolar ARs; B-type – irregular ARs that violate at least one of empiric rules; U-type – unipolar spots. We found that regular/irregular ARs make near a half/quarter of all ones. The A-type ARs are distributed evenly between two maxima of each cycle, whereas the number of B-type ARs increases in the second maxima. Both regular and irregular ARs exhibit strong N-S-asymmetry. The number of A-type ARs in different hemispheres shows peaks in two maxima of each cycle alternatively (the sequence is different in studied cycles). The B-type ARs shows a similar pattern (although the A-peaks and B-peaks occurs in different cycle maxima), excluding immense B-peak in the S-hemisphere in the second maximum (cycle 24) that breaks the expected sequence. The cyclic variations of the normalized asymmetry index shows postponement for the B-type ARs (related to the S-hemisphere) with time difference ~1.5-2 years. The tendencies found are discussed in terms of the mean-field dynamo theory. The classification of ARs by AZh was supported by the RSF (Project 18-12-00131). VA thanks the MSHE of RF (Research 0831-2019-0006). The work of AKh was supported by the basic financial program of the FSR II.16. AKh thanks the support of the RFBRs grant 19-52-45002.
We present a catalog of bipolar active regions (ARs) violating Hale's polarity law over the period 1989–2018. The catalog is compiled based on visual inspection of solar data in web applications Debrecen Photoheliographic Data, Helioviewer and Solar Monitor. Also, data from catalogs of the Mount Wilson Observatory, Crimean Astrophysical Observatory (CrAO) and USAF/NOAA SRS were used. The compiled catalog includes bipolar ARs reverse to Hale's polarity law with sunspots/pores of both polarities and magnetic couplings between opposite polarities (in cases with available EUV data). Ambiguous and complex cases of ARs with violation of Hale’s polarity law included in the catalog are labeled with special marks. The catalog contains 275 ARs. This is about 3% of all observed ARs. For each AR, there are three information blocks in the catalog: USAF/NOAA SRS data, DPD data, and our special marks. The first and second blocks include data at the maximum of AR evolution (at the maximum of the area of sunspots). The catalog is available at the CrAO website https://sun.crao.ru/databases/catalog-anti-hale/. For details, see Zhukova et al. (2020, Solar Physics, Volume 295, Issue 12, article id 165). The AR classification by AZh was supported by RSF (Project 18-12-00131). VA is grateful to MSHE of RF (Research 0831-2019-0006). AKh is grateful to RFBR for awarding grant 19-52-45002.
We investigate how representing active regions with bipolar magnetic regions (BMRs) affects the end-of-cycle polar field predicted by the surface flux transport model. Our study is based on a new database of BMRs derived from the SDO/HMI active region patch data between 2010 and 2020. An automated code is developed for fitting each active region patch with a BMR, matching both the magnetic flux and axial dipole moment of the region and removing repeat observations of the same region. By comparing the predicted evolution of each of the 1090 BMRs with the predicted evolution of their original active region patches, we show that the bipolar approximation leads to a 24% overestimate of the net axial dipole moment, given the same flow parameters. This is caused by neglecting the more complex multipolar and/or asymmetric magnetic structures of many of the real active regions, and may explain why previous flux transport models had to reduce BMR tilt angles to obtain realistic polar fields. Our BMR database and the Python code to extract it are freely available.
In various classes of dynamo models, spot-producing magnetic fields are generated as axisymmetric toroidal flux-ropes. While mean-field models produce axisymmetric broad toroidal fields, full 3D convective models produce axisymmetric toroidal wreaths. All these models can reproduce various longitude-averaged features, such as solar-like butterfly diagrams. In recent simulations, we show that time-dependent non-axisymmetric m=1 type flows can originate due to nonlinear hydrodynamics of differential rotation. This non-axisymmetric flows will affect the axisymmetric meridional circulation, causing time-dependence in the reverse flow cell. We show that a dynamo, operating with such a time-dependent meridional circulation can explain the short-term variability (with periods of the order of a month) in the evolution of faculae around 75-degree latitudes, which have very recently been observed. We present results from various simulation experiments to determine what model conditions best-simulate the facular evolution. We also compare our results with the observations of surface active regions' evolutions as revealed from magnetograms.
The regular observation of the solar magnetic field is available only for about last five cycles. Thus, to understand the origin of the variation of the solar magnetic field, it is essential to reconstruct the magnetic field for the past cycles, utilizing other datasets. Long-term uniform observations for the past 100 years as recorded at the Kodaikanal Solar Observatory (KoSO) provide such an opportunity. We develop a method for the reconstruction of the solar magnetic field using the synoptic observations of the Sun's emission in the Ca IIK and H$\alpha$ lines from KoSO for the first time. The reconstruction method is based on the facts that the Ca II K intensity correlates well with the unsigned magnetic flux, while the sign of the flux is derived from the corresponding H$\alpha$ map which provides the information of the dominant polarities. Based on this reconstructed magnetic map, we study the evolution of the magnetic field in Cycles 15--19. We also study bipolar magnetic regions (BMRs) and their remnant flux surges in their causal relation. Time-latitude analysis of the reconstructed magnetic flux provides an overall view of magnetic field evolution. We identify the reversals of the polar field and critical surges of following and leading polarities. We found that the poleward transport of opposite polarities led to multiple changes of the dominant magnetic polarities in poles. Furthermore, the remnant flux surges that occur between adjacent 11-year cycles reveal physical connections between them.
We use statistical tools to analyse data from HMI to determine the magnetic flux distribution of photospheric magnetic features and its variation over a solar cycle. The nature of the observed flux distributions at different times during the solar cycle could be used to try and infer information about magnetic field generation mechanisms. In particular we compare whether the magnetic flux distributions are represented by a single power law or whether other distribution functions can provide a better representation of the data.
We find that the hypothesis that the distribution of observed photospheric fluxes follows a single power law over the full solar cycle cannot be discounted and investigate how the power law distribution changes over the solar cycle . We also consider whether a 'double' power law distribution could actually be more reasonable than that of a single power law. We also discuss potential implications of a double power law distribution for solar magnetic field generation.
Flux ropes are known to be a critical structure in flaring, jet formation and coronal mass ejections. They can be observed in sigmoidal emission structures and are frequently found in magnetic extrapolations. Two leading theories for their formation are the emergence of pre-twisted magnetic structures from the convection zone and formation above the photosphere due to driving motions around the polarity inversion line. To the best of our knowledge there exists not direct (observational) evidence to conclusively demonstrate on or the other mechanism is responsible for flux rope formation; evidence is generally indirectly obtained by modelling. In this talk I will introduce the concept of magnetic winding, a measure of the entanglement of the magnetic field which can be applied to magnetogram data to directly infer the structure of the emerging field. We demonstrate conclusively with a number of examples that a pre-twisted magnetic field emerges from the convection zone. We anticipate the magnetic winding will become a staple quantity in the interpretation of magnetic field structure from magnetogram data.
Recent observations from Parker Solar Probe and Solar Orbiter have emphasised the importance of small and short-lived phenomena in the solar atmosphere. The former has revealed a highly dynamic structure in the solar wind’s magnetic field, which are referred to as switchbacks. The latter has shown small extreme-ultraviolet brightenings in the solar corona, which were labelled campfires.
We have analysed 14 coronal upflows, which were derived as blue shifts in spectroscopic data and examined the potential sources for each upflow. This was done by using Hinode/EIS rasters and calculating the Doppler velocities for the Fe XII line. Then events, which are stronger blue-shifted than -6 km/s were extracted. Those blue-shift events in Hinode/EIS were then compared to SDO/AIA data in all extreme-ultraviolet wavelength bands. We could identify sources for 12 out of 14 events. Besides classical jets, four events are associated with bright points and seven events are connected to small scale sources. They are either short and faint brightenings or eruptions. Those small-scale events usually last for less than 25 minutes. In a last step those events were examined in Hinode/XRT and SDO/HMI data to get a better understanding.
Our work has shown that small-scale features, which are so faint and short-lived that they would usually be missed in imaging data can produce strong upflows. Their driving mechanisms and potential contribution to the solar wind however is not understood yet.
Various processes have been proposed to explain the heating of loops to coronal temperatures, from braiding of magnetic flux tubes to waves. The relative contribution of different heating mechanisms is yet to be determined.
We study the coupling of a coronal loop to the solar surface and the transport and deposition of energy in different atmospheric layers.
Using 3D MHD simulations with the MURaM code, we model a coronal loop as a straightened-out magnetic flux tube. At each footpoint, the loop is rooted in a shallow convection zone layer, leading to self-consistent heating by magnetoconvection.
Energy transport may occur through slow, relative motions of magnetic flux tubes or by small-scale motions within magnetic flux concentrations. We compare the contribution of flows on various spatial and temporal scales to the energy transport.
We find that a large part of the energy injected into the loop is generated by internal coherent motions within strong flux tubes.
Small-scale vortices are ubiquitous in the intergranular lanes in the photosphere. These structures extend through the chromosphere into the corona and transport a significant fraction of the Poynting flux into the upper atmosphere and show enhanced heating rates.
The energy deposition in the corona gives rise to a clear substructure in the emission showing strands with widths of a few hundred km.
Our model allows us to follow the energy from its origin in the convection zone to dissipation in the corona and the resulting synthetic emission.
Researchers in high-resolution solar physics should have access to research infrastructures that would otherwise be closed to them. That is the goal of the SOLARNET Trans-national Access programme which is funded by the European Union’s Horizon 2020 programme. The facilities include ground-based solar telescopes on the Canary Islands: GREGOR, SST, THEMIS, and VTT. In addition there is the SUNRISE 3 balloon mission, due to be launched in June 2022, and the Piz Daint supercomputer.
I will present the programme, introduce the participating facilities, explain the rules, and discuss the experience so far from the point of view of users and operators. Finally some words on the future.
Surges are dynamic, cool and dense ejections typically observed in chromospheric lines and closely related to other solar phenomena like UV-bursts or coronal jets. Even though surges have been observed for decades now, fundamental questions regarding the temperature and density distribution, as well as their connection and impact on upper layers of the solar atmosphere remain open. Our aim is to characterize the chromospheric and transition region properties of these phenomena taking advantage of high-resolution observations combined with advanced techniques. We have analyzed four surges that appear related to UV-bursts observed with the Interface Region Imaging Spectrograph (IRIS) on 2016 April. We have studied the mid- and low-chromosphere of the surges by getting their representative Mg II h&k line profiles through the k-means algorithm and performing inversions on them using the STIC code. We have also studied the far-UV spectra, focusing on the O IV 1399.8 and 1401.2 Å lines, and carrying out density diagnostics. We obtain that the mid- and low-chromosphere of the surges are characterized by temperatures between 5.5 and 6.9 kK, electronic number densities from $\sim 1.5\times 10^{11}$ to $2.5\times10^{12}$ cm$^{-3}$, and line-of-sight velocities of a few km/s at optical depths ranging from $\log_{10}(\tau)=-6.0$ to $-3.2$. We find, for the first time, observational evidence of O IV emission within the surges, indicating that these phenomena have a transition region counterpart even in the weakest lines. The O IV emitting layers of the surges have an electron number density between $2.5\times 10^{10}$ and $10^{12}$ cm$^{-3}$.
On January $18$, $2021$, Solar Orbiter (SolO) and Parker Solar Probe (PSP) were for the first time in a special orbital configuration, that is, in quadrature. At this time when traveling along its orbit very close to the Sun, PSP has been crossing the atmosphere of the Sun at a distance just above $20$ R$_{\odot}$. Because of the continuous expansion of the solar corona, the plasma crossed by PSP, which is moving outward at a speed above $100-200$ km s$^{-1}$ on the solar equatorial plane, is the same plasma observed with the Metis coronagraph just a few hours earlier at a distance of $3-7$ R$_{\odot}$ from the solar limb. It is, thus, the first time that the expanding coronal plasma - that is, the solar wind - fully characterized by observations remotely performed with Metis, encounters almost immediately in its way outward a suite of in-situ instruments that can directly measure its physical properties. This work deals with the joint SolO-PSP observations to study the transition of the solar wind plasma from the sub-Alfvénic solar corona to a region just above the Alfvén radius, thus aiming to investigate the evolution of the pristine solar wind not yet reprocessed by nonlinear interactions.
We present results of the first high cadence image sequence of the Extreme Ultraviolet Imager (EUI) taken on 2020 May 30, when Solar Orbiter was 31.5 degrees in solar longitude separated from Earth & SDO, and at 0.56AU from the Sun. At this distance, the two-pixel spatial resolution of EUI’s High Resolution EUV Telescope (HRIEUV) was 400 km. HRIEUV observed a quiet Sun region and detected small localised brightenings, nicknamed ’campfires’, with length scales between 400 km and 4000 km and durations between 10 sec and 200 sec. The smallest and weakest of these HRIEUV brightenings have not been previously observed. Simultaneous observations from the EUI High-resolution Lyman-α telescope (HRILYA) do not show localised brightening events, but the locations of the HRIEUV events clearly correspond to the chromospheric network. Comparisons with simultaneous AIA images shows that most events can also be identified in the 17.1 nm, 19.3 nm, 21.1 nm, and 30.4 nm pass-bands of AIA, although they appear weaker and blurred. Our differential emission measure (DEM) analysis indicated coronal temperatures. We determined the height for a few of these campfires to be between 1 and 5 Mm above the photosphere. We interpret these events as a new extension to the flare-microflare-nanoflare family. Given their low height, the EUI ‘campfires’ could stand as a new element of the fine structure of the transition region-low corona, that is, as apexes of small-scale loops that undergo internal heating all the way up to coronal temperatures.
During Solar Minimum, the Sun is relatively inactive with few sunspots observed on the solar surface. Consequently, we observe a smaller number of highly energetic events such as solar flares or coronal mass ejections (CMEs), which are often associated with active regions on the photosphere. Nonetheless, our magnetofrictional simulations during the minimum period suggest that the solar corona is still dynamically evolving in response to the large-scale shearing velocities on the solar surface. The non-potential evolution of the corona leads to the accumulation of magnetic free energy and helicity, which is periodically shed in eruptive events. We find that these events fall into two distinct classes. One set of events are caused by eruption and ejection of low-lying coronal flux ropes and could explain the origin of occasional CMEs during Solar Minimum. The other set of events are not driven by destabilisation of low-lying structures but rather by eruption of overlying sheared arcades. These could be associated with streamer blowouts which are often considered as potential candidates for stealth CMEs. The two classes differ significantly in the amount of magnetic flux and helicity shed through the outer coronal boundary. We additionally explore how other measurables such as current, open magnetic flux, free energy, coronal holes, and the horizontal component of the magnetic field on the outer model boundary vary during the two classes of event. This study emphasises the importance and necessity of understanding the dynamics of the coronal magnetic field during Solar Minimum.
The stellar atmospheric simulation code $\textit{Bifrost}$ is useful for exploring the plasma dynamics of the solar atmosphere, but also for tracking magnetically energetic events that may be efficient in heating the chromosphere and corona. In this study, a cube of quiet Sun was modeled in order to track a) the evolution of quiet Sun photosphere and atmosphere, and b) the effect of a horizontal magnetic flux sheet inserted at the bottom boundary of the computational box, located 2.5 Mm beneath the Solar surface. Before the horizontal flux insertion, a significant magnetic heating event took place in the simulation. The characteristics of this heating event are presented including time series of Joule and viscous heating, magnetic field properties, and plasma velocities. Magnetic field lines are traced in order to understand the topology of the field responsible for the heating, and the field geometry appears to be a bipolar loop with kG-strength footpoints in the photosphere. This bipolar loop is associated with a plasma bubble that extends to roughly 7 Mm above the Solar surface. Analysis of the Joule and viscous heating parameters indicates that a significant amount of heating occurs in the atmosphere when the loop and its associated plasma bubble collapse. A newly-developed test particle module in $\textit{Bifrost}$ called $\texttt{corks}$ is employed in order to accurately trace the evolution of this magnetic feature from conception to collapse, and the associated heating may provide insight into how bipolar magnetic features can contribute to atmospheric heating, even in the quiet Sun.
The High-Resolution Coronal Imager (Hi-C) was launched for a third time on 29th May 2018, resulting in 329 s of 17.2 nm data of target active region AR 12712 with a cadence of approx. 4 s, and a plate scale of 0.129 arcsec^2/pixel.
Co-aligned with SDO/AIA 17.1nm observations, this presentation outlines investigations of the widths of 49 coronal structures. Firstly, evidence of substructure within the loops that is not detected by AIA will be demonstrated. Hi-C 2.1 can resolve individual sub-loop strands as small as approx. 202 km, though the more typical strand widths seen are around 513 km. Strands from a region of low emission that can only be visualized against the contrast of the darker, underlying moss reveal the corona is filled with ubiquitous, low emission, low density magnetic threads.
Secondly, even at these spatial scales there may be evidence for further substructuring within the HiC strands themselves. Width profile intensity variations are reproduced by fitting multiple Gaussian profiles; 183 sub-elements are examined and most frequent structural widths are about 450–575 km with 47% of the strand widths beneath SDO/AIA resolution. These appear to be the result of multiple strands along the integrated line of sight rather than being the consequence of even finer sub-resolution elements.
Finally, the change of strand width along strand length is examined – open fan magnetic strand structures display a width increase from the base while closed structures show little variation. The implications of these results on coronal loop modelling will be discussed.
The role of magnetic fields in the chromospheric heating problem remains greatly unconstrained. Most theoretical predictions from numerical models rely on a magnetic configuration, field strength, and connectivity; the details of which have not been well established with observational studies for many chromospheric scenarios. High-resolution studies of chromospheric magnetic fields in plage are very scarce or non existent in general.
Our aim is to study the stratification of the magnetic field vector in plage regions. Previous studies predict the presence of a magnetic canopy in the chromosphere that has not yet been studied with full-Stokes observations. We use high-spatial resolution full-Stokes observations acquired with the CRisp Imaging Spectro-Polarimeter (CRISP) at the Swedish 1-m Solar Telescope in the Mg I 5173 Å, Na I 5896 Å and Ca II 8542 Å lines.
We have developed a spatially-regularized weak-field approximation (WFA) method, based on the idea of spatial regularization. This method allows for a fast computation of magnetic field maps for an extended field of view. The fidelity of this new technique has been assessed using a snapshot from a realistic 3D magnetohydrodynamics simulation.
With the advent of next generation high resolution telescopes, our understanding of how the magnetic field is organized in the internetwork (IN) photosphere is likely to advance significantly. We present high spatio-temporal resolution observations that reveal the dynamics of two disk-centre IN regions taken by the GREGOR Infrared Spectrograph Integral Field Unit (GRIS-IFU) with the highly magnetically sensitive photospheric Fe I line at 15648.52 Å. We apply inversions with the Stokes inversions based on response functions (SIR) code to retrieve the parameters characterizing the atmosphere, tracking the dynamics of small-scale magnetic features. We find linear polarization features (LPFs) with magnetic flux density 130−150 G and find LPFs appear preferentially at granule-intergranular lane boundaries. The weak magnetic field appears to be organized in terms of complex ‘loop-like’ structures, with transverse fields often flanked by opposite polarity longitudinal fields. We use snapshots produced from high resolution three-dimensional magnetohydrodynamic (MHD) simulations and employ SIR to produce synthetic observables in the same spectral window as observed by the GRIS-IFU. We then use a parallelized wrapper to SIR to perform nearly 14 million inversions of the synthetic spectra to test how well the `true' MHD atmospheric parameters can be constrained statistically. Finally, we degrade the synthetic Stokes vector spectrally and spatially to GREGOR resolutions and consider the impact of stray light, spatial resolution and signal-to-noise. We studied a LPF exhibiting very similar magnetic flux density as those observed by the GRIS-IFU. Thus, we demonstrate that MHD simulations are capable of showing close agreement with observations.
High-resolution UV observations of the solar atmosphere, complemented by photospheric measurements conveying information about the magnetic configuration of the region of interest, allow us to investigate the magnetic and plasma processes that drive coronal heating and energy release.
Here, we report on small-scale flux emergence and flux cancellation events and on the energy release phenomena simultaneously observed in coordinated campaigns involving ground- and space-based observatories (e.g., SST, IBIS, Hinode, SDO), focusing on recent results obtained by the IRIS satellite.
We discuss our findings illustrating how magnetic reconnection can explain the occurrence of such small-scale energetic events and how they are expected to be improved with upcoming observations from next-generation space missions, like Solar Orbiter and EUVST.
The Nuclear Spectroscopic Telescope Array (NuSTAR) is a hard X-ray focusing telescope designed to observe astrophysical sources, but with the capability of observing the Sun. NuSTAR’s higher sensitivity in the HXR range compared to previous solar X-ray instruments, such as RHESSI, combined with the recent solar minimum has provided a unique opportunity to study the faint HXR emission from features on the quiet Sun. We present analysis of such features from several of the NuSTAR quiet Sun observations from the recent minimum. The X-ray spectra of these events have been fit, allowing their temperatures and emission measures to be determined. The contribution of these faint features to heating the solar atmosphere is investigated by finding the highest temperatures they can reach, as well as searching for the presence of any non-thermal emission. In order to study the multithermal emission from the features, the NuSTAR results are combined with corresponding observations from SDO/AIA and Hinode/XRT to produce Differential Emission Measures.
We analyse quasi-periodic pulsations (QPPs) which happened about 25 minutes after an M4-class solar flare on 5 September 2017. The QPP event was manifested as a bursty rapid enhancement of the flare microwave and decimeter radio emission, with almost no signatures pronounced in soft X-rays in comparison with the background flux caused by the decay phase of the preceding M4 flare. Simultaneous observations of this event with the two radioheliographs of a new generation — the Siberian Radioheliograph (4–8 GHz) and the MUSER radioheliograph (0.4–2 GHz) — reveal the presence of QPPs which were co-existing in the microwave and decimeter bands. Quasi-periodic narrow-band bursts at 0.4–0.8 GHz with a characteristic timescale of about 5 s and a fine structure inside each burst are seen in the coherent emission. In the 4–8 GHz band, we detect QPPs of the non-coherent emission, with a longer period that decreases gradually from 35 s to 25 s during the event. The work aims to identify the presence or absence of a connection between these two types of QPPs by analysing their temporal features in the two types of emission, as well as analysing the available spectral and spatial information. Based on this analysis, the most likely scenarios for the event are discussed.
Fast electron streams in the plasma of the solar corona propagating along the magnetic field lines are able to drive Langmuir turbulence. The further resonant interaction of electrons with turbulent spectrum can lead to acceleration to high energies forming tails of a suprathermal distribution. Similar phenomena are observed in experiments at open magnetic traps with electron beams. An open magnetic trap for plasma confinement, to put it simply, is a magnetic configuration in which magnetic field lines are not closed and plasma can flow freely along them. Among other approaches, electron beams are used to create and heat plasma. Consequently, such a configuration may be interesting not only from the point of view of plasma confinement, but also for modeling some astrophysical phenomena occurring in the solar corona. In particular, the results of one such experiments at Gas Dynamic Trap (GDT) facility [1] are reported. In the experiment, electrons accelerated to energies an order of magnitude higher than the initial beam energy are observed. For the obtained results to be interpreted, the series of numerical particle-in-cell simulations with a continuously injected electron beam are carried out. It is demonstrated that with injection of a 30 keV electron beam in a plasma accelerated electrons achieve about 100 keV energies, power-law distribution of a suprathermal component are obtained. An interpretation of the presented results is given.
[1] Ivanov, A. A., Prikhodko, V. V. (2013). Plasma Physics and Controlled Fusion, 55(6), 063001.
Photospheric motions drive the twisting and braiding of coronal magnetic field confining loop plasma. Magnetic stress eventually leads to reconnection and conversion of magnetic energy into heat through current dissipation. We model this process by fully 3D MHD loop simulations and derive observables that directly track the dissipating currents, therefore providing evidence for the structuring and timing of the energy release and constraints for the observations.
The proton energy spectra of 23 Energetic Storm Particle events, occurring either in association with (16 events) or in absence of (7 events) Solar Energetic Particles, are investigated by using data from particle instruments aboard STEREO A in the energy range from 84.1 keV to 100 MeV. For the SEP events at quasi-perpendicular shocks, the Weibull distribution provides good fits to the spectra, over the whole energy range for some events, and only at high energies for the others, being lower energies explained by the power law predicted by the DSA. Instead, the SEP spectra at quasi-parallel shocks are better reproduced by a double power law. In the cases non associated with SEPs, an Ellison-Ramaty form fits the observed spectra. Moreover, a significant correlation of the downstream turbulence level is found with the Weibull parameters for quasi-perpendicular shocks, and with the proton peak value in the intermediate energy range 4-6 MeV for all the 16 shocks. Our results suggest that the downstream turbulence is a relevant factor in particle acceleration and that stochastic acceleration can be a plausible mechanism for re-acceleration at interplanetary shocks.
The launch of the Solar Orbiter mission has motivated an intensification of the science activities in preparation for the exploitation of the data. For the METIS coronagraph, these activities are coordinated by topical teams, working on different physical problems. Here we present the activities carried out so far by the topical team on Coronal Shocks and Particle Acceleration. This team is trying to find the answer to some of the Solar Orbiter scientific objectives, like how and where do shocks form in the corona, and how and where are energetic particles accelerated at the Sun. In this poster, we will give an overview of the talks delivered up to now on coronal shock observations, shock 3D reconstruction, solar energetic particles, solar radio observations, shock acceleration, modelling and numerical simulations, and synergy with other instruments and other space missions.
On February 12, 2021 two subsequent eruptions occurred above the West limb, as seen along the Sun-Earth line. The first event appeared in the SOHO/LASCO-C2 images as a typical Coronal Mass Ejection (CME), starting around 12:48 UT with a projected speed on the order of 120 km/s, as provided by CACTUS catalog. This slow CME was followed ~7 hours later by a smaller and collimated prominence eruption, originating Southward with respect to the CME, and propagating much faster at ~380 km/s. Interestingly, these two events were also observed not only by STEREO-A, but also by remote sensing instruments on-board Solar Orbiter, located at about 163 deg of separation angle from the Earth, hence observed the eruptions above the East limb. The two events were first observed by the SoloEUI imager, then crossed the field-of-view of the SoloMetis coronagraph, being finally observed by the SoloHI instrument. From the Solar Orbiter perspective the different source regions of the two eruptions were located just behind the limb, as suggested by SDO/AIA images, but the EUI imager followed very well the expansion of the prominence eruption. The Metis images show both in the VL and UV channels a faint but classical three-part structure CME, followed by a brighter plasma blob associated with the prominence eruption. The southward part of the CME was also observed higher up by SoloHI, while the prominence eruption (expanding more northward) was probably missed. This presentation will summarize the first results from the analysis of these two interesting events.
Working towards improved space weather predictions, we aim to quantify how the critical height at which the torus instability drives coronal mass ejections (CMEs) varies over time in a sample of solar active regions. We model the coronal magnetic fields of 37 bipolar active regions and quantify the critical height at their central polarity inversion lines throughout their lifetimes. We then compare these heights to the changing magnetic flux at the photospheric boundary and identify CMEs in these regions. When the magnetic flux of an active region increases due to the continuous emergence of a single bipole, the critical height tends to increase, whereas the emergence of a new bipole into an existing active region or quiet Sun environment often causes the critical height to decrease sharply. A similar invesitgation of periods of decreasing magnetic flux indicates that the critical height rises when magnetic concentrations disperse, and falls when polarities converge and cancel at their inversion line. These results support and extend previous studies by showing that the average critical height is generally proportional to the separation between active region sunspots through time. We find higher rates of CMEs at times when the critical height is falling rather than rising, and when magnetic flux is increasing rather than decreasing. With continued work to also study multipolar regions, we may be able to identify conditions that are more conducive to producing eruptions, and determine the relative likelihood of active regions producing CMEs using readily-available observational proxies.
Solar eruptive events entail a complex interplay of energy release, transport, and conversion processes. A quantitative characterization of the different forms of energy therefore represents a crucial observational constraint for models of solar eruptions in general, as well as for magnetic reconnection, heating, and particle-acceleration processes in particular. These constraints are derived from X-ray, EUV and bolometric observations. We first review the results of recent statistical studies, focusing on possible explanations for apparent discrepancies between the different studies. We then present some of the first results on energy partition obtained with the novel STIX X-ray spectrometer/imager on Solar Orbiter. Finally, we present the first upper limits on energy input by nonthermal electrons given by the warm-target model.
Coronal Mass Ejections (CMEs) are large-scale eruptions expanding all the way from the low corona into the interplanetary space. Despite CMEs are spectacular events and attract wide interest among scientists and general public, these phenomena can seriously impact the Earth and potentially damage human facilities. CMEs have been studied quite extensively since their discovery, however different aspects governing this type of event still need to be understood.
From this perspective, the GOES M3.9 flare occurred on 2021 May 7 provides us with the unique set of observations to study the origin and the dynamics of its related fast CME and EUV wave. While the STIX instrument (Spectrometer/Telescope for Imaging X-rays), the Hard X-Ray (HXR) telescope onboard Solar Orbiter, allows us to investigate the flare and correlate the flare-accelerated electrons with the eruption, the combined near simultaneous observations from three different locations in the heliosphere, from Solar Orbiter, STEREO A and Earth, give us also the opportunity to disentangle the morphology of the CME, track the origin and evolution of the eruption, and deduce the kinematics of both the CME and the associated EUV wave.
Information on electric fields in the photosphere is required to calculate the electromagnetic energy flux through the photosphere and set up boundary conditions for data-driven magnetohydrodynamic (MHD) simulations of solar eruptions. Recently, the PDFISS method for inversions of electric fields from a sequence of vector magnetograms and Doppler velocity measurements was improved to incorporate spherical geometry and a staggered-grid description of variables. The method was previously validated using synthetic data from anelastic MHD (ANMHD) simulations. We further validate the PDFISS method, using approximately one-hour long MHD simulation data of magnetic flux emergence from the upper convection zone into the solar atmosphere. We reconstruct photospheric electric fields and calculate the Poynting flux, and compare those to the actual values from the simulations. We find that the accuracy of the PDFISS reconstruction is quite good during the emergence phase of the simulated ephemeral active region evolution and decreases during the shearing phase. Analysing our results, we conclude that the more complex nature of the evolution (compared to the previously studied ANMHD case) that includes the shearing evolution phase is responsible for the obtained accuracy decrease.
Supra-arcade downflows (SADs) are tadpole-shaped dark voids that descend through the cusp-shaped field lines of the current sheet and observed throughout the prolonged flare decay phase. Therefore, probing the thermodynamical and magnetic nature of the SADs can offer new insights into the reconnection mechanism during the flare gradual phase. Here, we investigate six distinctively clear episodes of SADs observed during the decay phase of an M-class flare of April 11, 2013. Unlike previous SAD investigations mainly targeting the limb flares, the selected on-disk located flare (AR11719) offers a unique opportunity of probing the effects of the interaction of SADs with the post-flare loop arcade and foot-points. Besides known effects, such as the generation of transverse waves (Period~160s) in the supra-arcade field lines followed by the passing of the void, our analysis revealed new facts presented as follows. DEM analysis of the SAD cases that occurred close to the flare-maximum revealed to contain hot plasma of temperature 5-7 MK. SADs collision with the post-flare loop arcade resulted in hot plasma of 10 MK temperature at the collision site and generated EUV intensity perturbations expanding and propagating with a speed ~400 km/s. In contrast, striking signatures of foot-point brightening (AIA/SDO 1700Å) are observed immediately after the SAD’s interaction with cusp-shaped loops (time-delay 20-32 sec; perturbation propagation speed ~ 2100 km/s). Further, UV emission from the ribbon location exhibited a periodicity of 10-minute, similar to the SAD occurrence rate, thus indicating its definitive contribution in the often observed quasi-periodic nature of flare emission.
Coronal dimmings are sudden decreases of the solar EUV and X-ray emission caused by coronal mass ejection (CMEs). Dimming regions map to the bipolar ends of closed magnetic field lines that become stretched or temporarily opened during an eruption, and are a result of the depletion of coronal plasma caused by the expansion and mass loss due to the CME. Recently available multi-point imagery from satellites at different locations in the heliosphere provided us with unprecedented observations of the three-dimensional evolution of solar CMEs and their coronal dimmings. These studies showed distinct correlations between CME mass and speed with key parameters of the associated coronal dimmings such as their spatial extent and intensity drop (Dissauer+ 2019, Chikunova+ 2020). Here, we study Sun-as-a-star broad-band EUV light curves derived from SDO’s Extreme ultraviolet Variability Experiment (EVE) as a testbed to study whether coronal dimmings can be also observed on stars and used for stellar CME detection. We demonstrate that large eruptive flares are with a high probability associated with a post-flare coronal dimming, with intensity drops in the 15-25 nm full-Sun light curves up to 5%. Searching for similar patterns of post-flare dimmings in the X-ray and EUV light curves of solar-like and late-type stars, we identify 21 stellar CME candidates, which is more that all previous reports of stellar CMEs. The derived intensity drops are an order of magnitude larger than for the Sun, suggesting that a substantial part of the stellar corona gets ejected by the CME.
We present a statistical study on the early evolution of coronal mass ejections (CMEs), to better understand the effect of CME (over)-expansion and how it relates to the production of Solar Energetic Particle (SEP) events. We study the kinematic CME characteristics in terms of their radial and lateral expansion, from their early evolution in the Sun’s atmosphere as observed in EUV imagers and coronagraphs. The data covers 72 CMEs that occurred in the time range July 2010 to September 2012, where the twin STEREO spacecraft were in quasi-quadrature to the Sun-Earth line. From the STEREO point-of-view, the CMEs under study were observed close to the limb. We calculated the radial and lateral height (width) versus time profiles and derived the corresponding peak and mean velocities, accelerations, and angular expansion rates, with particular emphasis on the role of potential lateral overexpansion in the early CME evolution. We find high correlations between the radial and lateral CME velocities and accelerations. CMEs that are associated with SEPs tend to be located at the high-value end of the distributions of velocities, widths, and expansion rates compared to non-SEP-associated events.
Although the sources of the fast solar wind are known (the coronal holes), the exact acceleration mechanism of the fast solar wind is still not fully understood. An important factor that can improve our understanding is the combination of remote sensing and in-situ measurements.
In order to combine them, it is necessary to accurately identify the source location of the in-situ solar wind with a process called back-mapping. Back-mapping consists mainly of two parts.
The first one is the ballistic mapping where the solar wind radially draws the magnetic field into the Parker Spiral, down to a point in the outer corona.
The second one is the magnetic mapping where the solar wind follows the non-trivial magnetic field line topology down to the solar surface. The magnetic field in this region is derived from a global model, like the potential field source surface extrapolations (PFSS).
In this study we focus on this back-mapping of the fast solar wind and try to determine all the uncertainties and sources of error that can affect the final location deduced on the solar surface. We compare different models for the ballistic mapping and also for the magnetic mapping and explore which free parameters have the greatest effect in the back-mapped locations.
Finally, we provide an uncertainty estimation for the back-mapped footpoints and compare our results with existing frameworks, like the Connectivity-Tool of IRAP.
The strive for improving space weather forecasts naturally comes with the need for a standardized validation scheme for the involved models. Especially the performance of coronal (magnetic field) models that form the lower boundary of forecasting simulations is crucial as their errors are further propagated by solar wind models. We therefore developed a benchmarking system, allowing the quality assessment for solar coronal magnetic field models in an easy-to-implement manner. Our system is constructed as a step-wise scheme, incorporating 1) visual inspection with multi-view point white-light data, 2) magnetic topology analysis with EUV on-disk data and 3) a feature matching implementation, also using white-light data from multiple perspectives. The strength of our assessment scheme lies in both the multi-view point aspect as well as the combination of both topological on-disk as well as off-limb structure analysis, providing a very detailed insight into a models magnetic configuration. A broad applicability is ensured by the possibility for customization of the sub-steps, while providing the framework for comparison. To showcase its application, also to derive ideal parameter sets for the model(s) under investigation, we used the validation system on the coronal model of EUHFORIA. We hereby run the model with 67 different parameter configurations and derive the best performing parameter sets.
For forecasting the arrival of coronal mass ejections (CMEs) at Earth, heliospheric 3D models such as EUHFORIA (EUropean Heliospheric FORcasting Information Asset) [Pomoell and Poedts,2018] rely on the correct observational input of the initial, near-Sun CME parameters (e.g. latitude, longitude, velocity, angular width, etc). The input parameters can be obtained by fitting the structure of the CME while it is still close to the Sun (up to 21.5 solar radii) by using different reconstruction methods such as the Stereo CME Analysis Tool (StereoCAT) and the Graduated Cylindrical Shell (GCS).
The StereoCAT online tool calculates the 3D kinematic properties of CMEs by triangulating their features based on up to three different coronagraph fields-of-view under the assumption that CMEs present a circular cross-section and maintain a constant angular width during their radial expansion, the so-called “cone model” [Millward,2013].
On the other hand, the GCS model [Thernisien,2011], consists of two cones that represent the "legs", attached to the ends of a tubular section, together forming the main body. Like StereoCAT, this tool relies on two different white-light coronagraph fields-of-view for the fitting of the CME shape with no description for the inside structure.
In this study, 19 Earth-directed CME events were selected and their kinematic parameters were calculated using both StereoCat and GCS tools. The aim of this work is to compare the CME properties obtained by both methods and understand how their potential differences lead to different modeling results at Earth when we propagate the CME structures with EUHFORIA.
The EUropean Heliospheric FORecasting Information Asset (EUHFORIA, Pomoell and Poedts, 2018) is a physics-based heliospheric and CME propagation model designed for space weather forecasting and other scientific studies. Although EUHFORIA can predict the solar wind plasma and magnetic field parameters at Earth, it is not designed to evaluate geomagnetic indices like Disturbance-storm-time (Dst) or Auroral Electrojet (AE) that quantify the impact of the magnetized plasma encounters on Earth’s magnetosphere. Therefore, we coupled EUHFORIA with the Open Geospace General Circulation Model (OpenGGCM, Raeder et al, 1996), a magnetohydrodynamic model of Earth’s magnetosphere. In this coupling, OpenGGCM is driven with the synthetic solar wind and interplanetary magnetic field obtained from EUHFORIA simulations as input to produce the magnetospheric and ionospheric parameters of Earth. This coupling is validated with observed geo-effective CME events modelled with flux-rope CME models like Spheromak and FRi3D. We compare these simulation results with the indices obtained from OpenGGCM simulations driven by the measured solar wind data from spacecraft like WIND. We further discuss how the choice of CME model and observationally constrained parameters influence the input parameters, and hence the geomagnetic disturbance indices estimated by OpenGGCM. We also discuss some limitations of the coupling and suggest improvements for future work.
Time-series of historical solar irradiance variations is an important input to climate models. An extension of the record of direct irradiance measurements available since 1978 to earlier times is only possible with the help of models. For this, we need to know the evolution of the surface magnetic field. The longest record of direct observations of solar activity is the sunspot number covering the last four centuries. However, it has the shortcoming that it only allows tracing the evolution of the large-scale active region (ARs) harbouring sunspots, while the evolution of small-scale ephemeral regions (ERs) is heavily uncertain. At the same time, ERs play an important role in driving the long-term irradiance variations. We use a new model of the ERs emergence based on recent solar observations, where the emergence of all magnetic regions is described by a single power-law distribution with an exponent varying with solar activity, as represented by the sunspot number. The evolution of the magnetic field with time is simulated with a surface flux transport model, and the computed magnetic field is used to reconstruct solar irradiance.
The role of magnetic reconnection in the acceleration of coronal mass ejections (CMEs) has been widely discussed. However, because CMEs are found to have expansion speed which is comparable to propagation speed in the corona, it is still not clear about which portion of the reconnection contributes to the acceleration and expansion separately. To address this question, we analyze a fast CME event on 2013 February 27, associated with clearly observed three-part structure. We find that the CME front undergoes a smooth but long-lasting acceleration in the high corona while the speed of its core remains constant. This acceleration is caused by the additional CME expansion along the radial direction (with acceleration speed of Ae). Magnetic reconnection is found to occur after the eruption of the CME and to continue during the CME propagation. We estimate the potential acceleration caused by the drag-based model (Ad), in which the CME deceleration due to the solar wind drag is thought to be compensated by the acceleration via reconnection. The comparison between Ae and Ad reveals that the contribution of the magnetic reconnection in the high corona to the expansion is comparable to or larger than its contribution to the acceleration. The result also brings a view that the expansion shall be considered separately when studying CME dynamics.
The chromosphere is a very dynamic and complex layer where all the relevant physical processes happen on very small spatio-temporal scales. A few spectral lines that can be used as chromospheric diagnostics, give us convoluted information that is hard to interpret without realistic theoretical models. What are the key ingredients that these models need to contain? It is clear that what shapes the chromosphere and determines how and where the energy is deposited is the magnetic field configuration. In this review, we will discuss the formation and properties of chromospheric structures at different spatial scales. We will give an overview of what our models can reduce and what challenges we face. We will also touch on how chromospheric heating depends on emerging flux.
Observations of the Sun reveal a rich array of dynamics throughout all levels of the solar atmosphere. In many cases. the observed dynamic motions are driven by the magnetic field. However, the lower solar atmosphere, i.e. the photosphere and chromosphere, is a partially ionised plasma, with most of the species being neutral. This means that the driver of the fluid motions cannot directly influence the fluid itself, this only happens through the interaction of neutral and charged species. In this talk I will look at two areas of research into partially ionised plasma dynamics, relating to MHD shocks and instabilities, which are of particular relevance to our understanding of the dynamic solar atmosphere. For shocks, the neutral fluids decouples from the magnetic field in the shock front, creating a broad shock transition that contains substructure, and can influence the stability of the shock. For instabilities, partial ionisation is found to change the growth rate and the effects of non-linear transport. To date studies using two fluid models are often highly idealised, but progress is being made to look at more realistic settings. I will review some of the recent advances.
How mass is loaded into the upper chromosphere and transition region is an important unclosed matter. The standard fibrilar mass loading scenario is of feeding material up relatively static fieldlines by the guiding magnetic field, resulting from initial impulses made by p-mode oscillations (Hansteen et al 2006, De Pontieu et al 2007). Instrumentation such as DKIST and EST will provide an excellent opportunity to address this issue.
We use passive tracer particles seeded into dense fibrils in 3D RMHD Bifrost simulations to investigate fibril creation and destruction. The most common “lift and drain” mass loading scenario found is markedly different to previous suggestions. Box oscillations, the simulation equivalent of the p-modes initiate the formation. Rather than loading material up the footpoints of static fieldlines, the fieldlines themselves rise, firstly near the footpoints where the plasma velocity is well aligned with vertical fieldlines. Material is then caught above the flattened apexes of rising fieldlines and lifted by the Lorentz force along the central lengths of the fibrils as the fieldline untwists and becomes more parabolic. Subsequently, material drains into one or both footpoints under gravity. Instances are also found of material with horizontal velocities that are simultaneously elevated in rising fieldlines, creating the illusion of parabolic motion up a static fieldline.
These mechanisms are not implausible additional solar scenarios for fibrilar mass loading. Criteria for discerning between this and standard mass loading scenarios are described. Experimental parameters required to achieve more standard fibrilar mass loading in the simulations are discussed.
Atmospheric models place the Chromosphere-Corona Transition Region at $\sim2$Mm above the $\tau_{5000}=1$ level. Os course, the upper part of the chromosphere is highly inhomogeneous, with spicules intruding into the corona. There is, however, a more homogeneous lower region, as evidenced in the MgII triplet lines, extending to $\sim2$Mm (Alissandrakis etal.; https://doi.org/10.1007/s11207-018-1242-4). In SDO and TRACE images spicules appear in emission in the 1600, 1700 and 304A bands and in absorption in the EUV bands; the latter is due to photo-ionization of HI and HeI, which increases with wavelength. At the shortest available AIA wavelength and taking into account that the photospheric limb is $\sim0.34$Mm above the $\tau_{5000}=1$ level, we found that TR emission starts at $\sim3.7$Mm; extrapolating to $\lambda=0$, where there is no chromospheric absorption, we deduced a height of $3.0\pm0.5$Mm, above the value of 2.14Mm of Avrett and Loeser (2008,ApJS,175,229).
Another indicator of the extent of the chromosphere is the height of the network. This produces a limbward shift of features with respect to the position of their counterparts in magnetograms. Using this approach, we measured heights of $0.14\pm0.03$Mm(1700A), $0.39\pm0.06$Mm(1600A) and $3.29\pm0.23$Mm(304A), with a possible solar cycle variation.
A third indicator is the position of the limb in UV as well as in ALMA mm-λ images. This is not very reliable, as the limb position is affected by spicules, but it is indicative. We obtained values of $1.4\pm0.2$Mm(1600A), $2.4\pm0.7$Mm(ALMA 1.26mm), $4.2\pm2.5$Mm(ALMA 3mm) and $5.7\pm0.2$Mm(304A).
Putting everything together, we conclude that the average chromosphere extends higher than homogeneous models predict.
The Solar Orbiter mission of ESA and NASA is currently on a trajectory that will take it into the inner heliosphere from where it will explore the Sun (and heliosphere) from close up and from out of the ecliptic plane. It aims to address the overarching questions of how the Sun creates and controls the heliosphere, and why solar activity changes with time. Among the instruments that Solar Orbiter carries is the Polarimetric and Helioseismic Imager (SO/PHI), which is the first magnetograph to observe the Sun from outside the Sun-Earth line. Already the trajectory provides SO/PHI with unique capabilities, although it also poses huge challenges, which could only be overcome by technology developments on a significant scale. Although Solar Orbiter is still in cruise phase first glimpses of SO/PHI’s capabilities have become apparent, including the excellent quality of the data. The promise for the science that can be done with SO/PHI data in the future is immense, both with standalone observations by SO/PHI and with SO/PHI data combined with observations made by other Solar Orbiter instruments, or with data gathered by instruments on other spacecraft or on the ground. The talk will give a brief description of the Solar Orbiter mission, introduce the SO/PHI instrument, show first data and describe the science goals for the different phases of the Solar Orbiter mission. The SO/PHI data policy will also be briefly introduced.
Measurements of the magnetic field’s twist play an important role in constraining dynamo theory, models of flux emergence and the prediction of flares. We aim to characterize methods of measuring twist directly from SDO/HMI vector magnetograms by generating Monte-Carlo synthetic data sets. By studying several example sunspots we found that the temporal fluctuations in the HMI vector magnetograms are spatially correlated. We have developed an empirical model for noise that includes these spatial correlations.
We study the sunspot activity in relation to spotless days (SLDs) during the descending phase of solar cycle 11–24 to predict the amplitude of sunspot cycle 25. For this purpose, in addition to SLD, we also use the geomagnetic activity (aa index) during the descending phase of a given cycle. A very strong correlation of the SLD (R=0.68) and aa index(R=0.86) during the descending phase of a given cycle with the maximum amplitude of next solar cycle has been estimated. The empirical relationship led us to deduce the amplitude of cycle 25 to be 99.13± 14.97 and 104.23± 17.35 using SLD and aa index, respectively as predictors. Both the predictors provide comparable amplitude for solar cycle 25 and reveal that the solar cycle 25 will be weaker than cycle 24. Further we derive that the maximum of cycle 25 is likely to occur between February and March 2024. While the aa index has been used extensively in the past, this work establishes SLDs as another potential candidate for predicting the characteristics of the next cycle.
On a global scale chromospheric magnetic activity is represented by plages and enhanced chromospheric network. These phenomena significantly contribute to the variation of the solar UV radiation and the enhancement in chromospheric emission in the two strong resonance Ca II H & K lines. We present a set of excess brightness and area indices based on disk-resolved UV 1600Å images of the Atmospheric Imaging Assembly (AIA) on board the Solar Dynamics Observatory (SDO) and full-disk Ca II K line-core filtergrams of the Chromospheric Telescope (ChroTel) at Observatorio del Teide, Tenerife, Spain. In addition, we compute the spectroscopic S-index based on the quasi-synoptic observations in 2018 and 2019 with the Potsdam Echelle Polarimetric Spectroscopic Instrument (PEPSI) of the Large Binocular Telescope (LBT) at Mt. Graham International Observatory (MGIO), Arizona, U.S.A. All indices display signatures of rotational modulation, even during the very low magnetic activity in the minimum of Solar Cycle 24. The UV 1600Å and Ca II K image-based excess brightness indices reveal as strong peak of activity in 2012 and the double-peaked maximum in 2014. These features are driven by complex and large active regions. Furthermore, both spectral- and image-based indices demonstrate that the Solar Cycle 24 concludes with a deep minimum. Moreover, the SDO/AIA UV excess brightness indices reveal an intriguing aspect of activity asymmetry between the two hemispheres. In particular, starting in 2018, the rotational modulation in the southern hemisphere vanishes, indicating exceptionally low solar activity representing the basal activity level of the Sun.
Far-side helioseismology is a technique used to detect activity signatures in the far hemisphere of the Sun, based on near-side wave field interpretation. We evaluated the performance of a new neural network approach, developed to improve the sensitivity of the seismic maps to the presence of far-side active regions, and thoroughly compared it with the standard method commonly applied to predict far-side active regions from seismic measurements, using STEREO extreme ultraviolet observations of the far hemisphere as a proxy of activity.
We have confirmed the improved sensitivity of the neural network to the presence of far-side active regions. Approximately 96% of the active regions identified by the standard method with strength above the threshold commonly employed by previous analyses are related to locations with enhanced extreme ultraviolet emission. For the same percentage of false positives, the neural network can provide a 47% increase in the number of far-side active region detections confirmed by their extreme ultraviolet brightness. Weaker active regions can be detected by relaxing the threshold in their seismic signature. For almost all the range of thresholds, the neural network delivers a higher number of confirmed detections and a lower rate of false positives.
The neural network is a promising approach to improve the interpretation of the seismic maps provided by local helioseismic techniques, which can lead to improvements in space weather forecasting.
It is still an open question if the quiet Sun small-scale magnetic field mainly originates of a turbulent cascade acting on fields produced by a global-scale dynamo, or if it is mainly generated locally by a small-scale turbulent dynamo. Consequently, a number of numerical studies focusing on turbulent dynamos was carried out in the recent past. Despite of these works providing extremely useful information on many aspects of small-scale dynamo action, it is still unclear how to extrapolate these results to the Sun, in particular because of the disparate regimes of magnetic Prandtl numbers, $Pr_m$, between numerical simulations and the real Sun. The present work addresses these issues in a twofold way. First, a general methodology for estimating the effective diffusivities stemming from radiative MHD simulations is proposed. It is based on the method of Projection on Proper elements, initially introduced in the plasma physics community to verify plasma turbulence simulation codes. It relies on a post processing step using different, higher order accurate numerical operators. Second, a study of how the magnetic field resulting from small-scale solar dynamo simulations depends on the Reynolds number, $Re$, and magnetic Reynolds number, $Re_m$, is presented. For this, several radiative MHD simulations with different effective viscosity and plasma resistivity are carried out with the CO5BOLD code and the resulting magnetic energy growth rate and saturated magnetic field are characterized in terms of $Re$ and $Re_m$. It is shown that it is possible to simulate small-scale dynamo action also in the regime $Pr_m<1$.
This contribution describes the procedure by which we found relationship between the rotational velocity of the solar corona and the level of the solar activity (phase of the solar cycle) in the period of 2011 - 2020. The deviation of the speed from the mean value is ± 0.0239 °/day, which corresponds on the solar surface near the equator to ± 3.16 m/s, with a mean value of about 14.1 °/day (1864.3 m/s). The level of activity was determined using the coronal index (CI) and we used the data on coronal rotational velocity from our recent work (Dorotovič and Rybanský, 2019). The correlation coefficient between the monthly averages of the CI and the rotational velocity during the given period (120 months) is 0.752. We did not find theoretical explanation for this phenomenon.
Reference: Dorotovič, I., Rybanský, M. Rotation of Some Solar Coronal Bright Features as Derived from the Solar Dynamics Observatory/Atmospheric Imaging Array (SDO/AIA) 21.1 nm Images (for the Years 2011 – 2018). Sol. Phys. 294, 109 (2019). https://doi.org/10.1007/s11207-019-1501-z
Late-type stars often display multiple and variable levels of periodic magnetic activity. It is well established that our nearest stellar source, the Sun, manifests similar levels of magnetic activity, including the 11-year sunspot cycle discovered two centuries ago. This solar cycle dominates the properties of large-scale phenomena, such as flares and sunspots. However, little is known about how the solar cycle influences the dynamics of localized small-scale events. Here, we report our finding of the modulation of off-limb coronal jets by solar cycles on timescales of both 11 years and 1 year. The modulation is evidenced by the coronal jet butterfly diagram and the quasi-annual periodicities of their intensities, locations and structural characteristics. We also find a power-law distribution of the jet intensity, which is highly consistent with that found for solar and stellar flares. This suggests that the small-scale eruptive events studied here exhibit self-organized criticality similar to their large-scale counterparts.
Interchange reconnection has been proposed as a mechanism for the generation of the slow solar wind, and a key contributor to determining its characteristic qualities. We study the implications of interchange reconnection for the structure of the plasma and field in the heliosphere in the context of the "S-Web" model. We show that photospheric driving at supergranular scales leads to a corrugation (at low altitudes) of the separatrix surfaces that define the streamer and (to a lesser extent) the pseudostreamer. We demonstrate that newly-opened magnetic flux is distributed in a filamentary pattern in the heliosphere, suggesting that the pattern of granular and supergranular flows on the photosphere should leave an observable imprint in the heliosphere. As a result the connectivity of a heliospheric spacecraft trajectory to the photosphere exhibits high complexity.
Understanding processes in the quiet Sun is crucial for understanding the Sun in general. The overarching goal of our study is to quantify the energy output of the quiet Sun, which can be expressed in terms of the Poynting flux. To compute this quantity, one can use Maxwell's equations, provided the full orientation of magnetic, electric, and velocity fields are available. All of those can be recovered from spectropolarimetric data using different inversion methods.
Quiet Sun magnetic fields have only recently become observable with the launch of missions such as Hinode and SUNRISE. The Daniel K. Inouye Solar Telescope (DKIST) is expected to improve the quality of these observations even further. While the SUNRISE/IMaX images have a resolution of 0.15 ''/pixel, the DKIST ViSP instrument available in the first cycle will provide magnetograms with a resolution of 0.05''/pixel. The cadence of images provided by the VBI is 7 seconds compared to 12 seconds by IMaX. The signal-to-noise ratio of Stokes vectors measurements is likewise expected to improve.
We present our preliminary results obtained from velocity and electric field inversions of photospheric images, magnetograms and Doppler velocities from SUNRISE/IMaX, the challenges associated with these inversions, and implications for DKIST observations. Specifically, we use Fourier Local Correlation Tracking (FLCT) and machine-learning-based algorithm, DeepVel, to obtain, respectively, optical flows and velocity fields, and compare these with quantities derived using the PDFI electric-field inversion method.
The confluence of the data from the Murchison Widefield Array and an imaging pipeline tailored for spectroscopic snapshot images of the Sun at low radio frequencies have led to enormous improvements in the imaging quality of the Sun. These developments have lowered the detection threshold for nonthermal emissions by up to two orders of magnitude as compared to earlier studies, and enabled our discovery of Weak Impulsive Narrowband Quiet Sun Emissions (WINQSEs). In our studies we find WINQSEs to be consistent with the radio signatures of coronal nanoflares, hypothesized by Parker (1988) to explain coronal heating in the quiet Sun emissions. As a first step towards exploring this tantalising possibility of making progress on the coronal heating problem, we have been pursuing multiple projects to better understand the observational characteristics of WINQSEs. These include attempts to look for WINQSEs in multiple independent datasets; attempting to characterise their morphologies in radio maps using Artificial Intelligence/Machine Learning based approaches; understanding their spectro-temporal structure by making solar images with a time resolution of a few milliseconds and frequency resolution of ~100 kHz. Here we present the current status of these projects.
The third flight of the Sunrise observatory carries the new Sunrise UV Spectropolarimeter and Imager (SUSI) which will cover the spectral range from 310 nm to 410 nm. In this region, the number density of spectral lines is at least four times larger than in the visible/infrared part of the spectrum, including a significant number of chromospheric lines. To extract accurate physical parameters of the solar atmosphere from observations with SUSI we need precise atomic line parameters, e.g., the log (gf) value. Here we review an extension of the spectropolarimetric inversion scheme to account for coupled inversion of atomic line parameters. In this scheme, atomic line parameters are inverted using information from the whole field of view. Additionally, we discuss the potential of this inversion scheme using synthetic spectra computed from 3D realistic magnetohydrodynamic simulations.
Numerical and observational evidences both support that wave propagation and dissipation may be an important mechanism that contributes to the heating of the solar chromosphere. For instance, acoustic waves and the resulting shock waves in the gravitationally stratified solar atmosphere, may provide at least part of the energy to compensate the radiative energy losses in the chromosphere. However, high-frequency waves are difficult to observe because of the limited instrumental resolution, and in fact, numerical modelling also needs sufficient spatial and temporal resolution for high-frequency waves to avoid artificial numerical dissipation. Therefore, numerous one-dimensional numerical simulations have been performed without taking into account multi-dimensional effects, thus reducing the computational costs. We have used a neutral-ion two-fluid model to investigate high-frequency acoustic wave propagation in one-dimensional gravitationally stratified partially ionised plasmas, showing that sufficient energy can be transported from the bottom of the photosphere up to the chromosphere to compensate the radiative energy losses (Zhang et al. 2021). The model assumes an initial hydrostatic and ionisation equilibrium, and takes into account the effects of neutral-ion collisions, ionisation and recombination. In this work, we further quantify the multi-dimensional effects in modelling acoustic/shock wave propagation. More specifically, as our previous simulations show that the shock wave damping yields an important heating process, in two-dimensional simulations the formation of shocks may change since the energy spreads also in the horizontal direction as the waves propagate in the vertical direction.
Thermal non-equilibrium (TNE) produces several observables that can be used to constrain the spatial and temporal distribution of coronal heating. Its manifestations include prominence formation, coronal rain, and long-period intensity pulsations in coronal loops. The recent observation of abundant periodic coronal rain associated with intensity pulsations by Auchère et al. allows to unify these two phenomena as the result of TNE condensation and evaporation cycles. On the other hand, many intensity pulsation events observed by Froment et al. show little to no coronal rain formation. Our goal is to understand why some TNE cycles produce abundant coronal rain, while others produce little to no rain.
We reconstruct the geometry of the event reported by Auchère et al., using images from STEREO/SECCHI/EUVI and magnetograms from SDO/HMI. We then perform 1D hydrodynamic simulations of this event, for different different heating parameters and variations of the loop geometry (9000 simulations in total). We compare the resulting behaviour to simulations of TNE cycles by Froment et al. that do not produce coronal rain. Our simulations show that both prominences and TNE cycles (with and without coronal rain) can form within the same magnetic structure. We show that the formation of coronal rain during TNE cycles depends on the asymmetry of the loop and of the heating. Asymmetric loops are overall less likely to produce coronal rain, regardless of the heating. In symmetric loops, coronal rain forms when the heating is also symmetric. In asymmetric loops, rain forms only when the heating compensates the asymmetry.
We have carried out the first comprehensive investigation of enhanced line emission from molecular hydrogen, H$_{2}$ at 1333.79 Å, observed at flare ribbons in SOL2014-04-18T13:03. The cool H$_{2}$ emission is known to be fluorescently excited by Si IV 1402.77 Å UV radiation and provides a unique view of the temperature minimum region (TMR). Strong H$_{2}$ emission was observed when the Si IV 1402.77 Å emission was bright during the flare impulsive phase and gradual decay phase, but it dimmed during the GOES peak. H$_{2}$ line broadening showed non-thermal speeds in the range 7-18 km/s, possibly corresponding to turbulent plasma flows. Small red (blue) shifts, up to 1.8 (4.9) km/s were measured. The intensity ratio of Si IV 1393.76 Å and Si IV 1402.77 Å confirmed that plasma was optically thin to Si IV (where the ratio = 2) during the impulsive phase of the flare in locations where strong H$_{2}$ emission was observed. In contrast, the ratio differs from the optically thin value of 2 in parts of ribbons, indicating a role for opacity effects. A strong spatial and temporal correlation between H$_{2}$ and Si IV emission was evident supporting the notion that fluorescent excitation is responsible.
The Evershed flow is one of the most outstanding features observed in sunspot penumbrae. It is a plasma flow running along penumbral filaments radially outwards and towards the moat of sunspots. This flow was first observed more than a century ago. Nevertheless, in the past decade, observations have shown unusual counter Evershed flows (CEFs) that run in the opposite direction, towards the sunspot umbra. Until now, very few CEFs have been reported. Thus, CEFs are still thought to be extremely rare events. In this work, we followed 97 active regions for an average of 9.6 days using SDO/HMI observations. Our sample includes various types of sunspots, from the most simple $\alpha$-spots to the more complex $\delta-$groups of sunspots. We report the detection of 384 CEFs, showing that CEFs are far more frequent than their rarity in the literature suggests. However, CEFs are still sparse as they are observed in just 5.9% of the average observed time. We explain that the small number of reports of CEFs was due to incomplete coverage of active regions, which was overcome by continuous observations taken from space.
The solar corona is characterised by its puzzling multi-million degree component. On the other hand, observations in the last decade have shown that the corona also contains a large amount of coronal rain, 10-100 times cooler and denser than the surroundings. The properties of coronal rain are now known to be strongly linked to the coronal heating properties, but its origin, dynamics, and morphology are still not well understood. In particular, the spatial and temporal occurrence of coronal rain in an active region is unknown. In this study, we carry out an imaging and spectroscopic multi-wavelength statistical study of coronal rain observed in an active region off-limb with IRIS and AIA, spanning chromospheric to transition region temperatures. We use the Rolling Hough Transform (RHT) to automatically detect and measure the properties of coronal rain clumps. Over the 4.5 hr long observation, the entire coronal area in the plane-of-the-sky up to a height of 30-40 Mm is covered by coronal rain, suggesting a prevalence of thermal non-equilibrium (TNE). We estimate the fraction of coronal volume in TNE and the role of coronal rain in the mass and energy cycle. The rain is predominantly at chromospheric, suggesting complete catastrophic cooling, while not much difference is observed in the dynamics over the temperature range. A small subset of loops also exhibit long-period intensity pulsations. We discuss the spatio-temporal properties of the heating linked to this cooling behaviour.
We discuss the diagnostics of plasma jets in the solar corona from multiwavelength imaging observations in the microwave band. We present several events observed with RATAN-600, Siberian Radioheliograph, and Nobeyama Radioheliograph. Obtained data provide us with spatially resolved imaging information alongside microwave flux observations at several frequencies. To analyze the context information on the three-dimensional structure of the coronal magnetic field, we reconstruct the magnetic field in the lower corona from the SDO/HMI magnetograms and compare it with the magnetic field at the base of the corona derived from the RATAN-600 data. In this work we demonstrate that microwave observations of the events associated with coronal jets can (1) give insights into jet dynamics and excitation mechanisms and (2) provide important information on physical conditions in the corona of an active region where a jet is initiated and developed.
This work is supported by the Russian Foundation of Basic Research grant 18-29-21016.
High resolution observations have shown the ubiquity of Alfvénic waves in the solar atmosphere. Recently, torsional Alfvén waves in coronal flux tubes have been first detected. Here, we perform numerical simulations of torsional Alfvén waves and study their nonlinear evolution. We consider a cylindrical, radially inhomogeneous, and straight coronal magnetic flux tube that is line-tied at two rigid walls representing the solar photosphere. Standing torsional Alfvén waves are excited by perturbing the azimuthal component of the velocity. The nonlinear evolution of these waves is obtained with the PLUTO code, which solves the ideal MHD equations using a finite-volume formulation with adaptive mesh refinement. Initially, torsional Alfvén waves undergo the process of phase mixing owing to the transverse variation of density, generating small scales across the magnetic field direction. After only few periods of torsional waves, azimuthal shear flows trigger the Kelvin Helmholtz instability (KHi), and the flux tube is subsequently driven to a turbulent state. Turbulence is anisotropic and develops transversely only to the background magnetic field. After the onset of turbulence, the effective Reynolds number decreases in the flux tube much faster than in the initial linear stage governed by phase mixing alone. We conclude that the nonlinear evolution of torsional Alfvén waves, and the associated KHi, is a viable mechanism for the onset of turbulence in coronal loops. Turbulence can significantly speed up the generation of small scales previously initiated by phase mixing.
It has been stated for a long time that the solar atmospheric plasma is not in a neutral state nor in a fully ionized state. The solar plasma is composed of different species, and it can be considered that each of them behaves like a fluid interacting with the rest of the species via collisions. When the collisional coupling is strong, the plasma mostly behaves as a single fluid. If this coupling weakens in certain processes, there might be deviations between the dynamical and thermal properties of the different species. To detect ion-neutral effects, it is necessary to measure as accurately as possible the velocity of different species at the same spatial position and simultaneously. Our aim is the detection of non-ideal ion-neutral effects in the solar plasma. The best candidate targets for this goal are spicules, surges, and the lower part of prominences. For this study, we observed a quiet Sun solar prominence at the east limb in June 2017 with the German Vacuum Tower Telescope. We acquired simultaneous spectra of the Ca II 8542 Å, Hα 6562.8 Å, and He D3 5875.6 Å lines. The spectroscopic mode of the spectrograph was chosen to ensure the high cadence and signal to noise needed to detect these effects and shed light on the scientific questions proposed.
The Fe I 6301.5 Å and 6302.5 Å lines are widely used to probe the solar photosphere. They are known to be affected by the non-local thermodynamic equilibrium (NLTE) conditions due to the ultraviolet overionisation of iron atoms in the solar atmosphere. This leads to deviations in their level populations based on Saha-Boltzmann statistics. When inverting their Stokes profiles to determine atmospheric parameters, the NLTE effects are often neglected and other quantities are tweaked to compensate for deviations from the LTE. In this work, we discuss how the routinely employed LTE inversion introduces errors in the derived atmospheric quantities. We show that when the NLTE effects are neglected, these errors can be as high as 13% in temperature, and in line-of-sight velocity and magnetic field strength the errors can even exceed 50%. Errors are found at the sites of granules, intergranular lanes, magnetic elements, and basically in every region with strong vertical gradients in the atmosphere. Similarly, strong horizontal gradients in temperature introduces 3D effects in these lines. We find that errors due to neglecting the 3D effects are more localised and are lower than 5% in temperature, and lower than 20% in both velocity and magnetic field strength. The NLTE and 3D effects are found to persist when the Stokes profiles are spatially and spectrally degraded to the resolution of the SST or DKIST. Our findings have wide-ranging consequences since many results derived in solar physics are based on inversions of these Fe I lines carried out in LTE.
Many processes in the solar atmosphere and in the solar wind require a kinetic description. Additionally the latest missions, SolO and PSP, provide new unique view of kinetic processes. We report here the approach of the Horizon 2020 project AIDA (www.aida-space.eu): using a combination of massively parallel kinetic particle in cell simulations and machine learning data mining. The study of kinetic processes provide large data sets: for example a massively parallel PIC simulation of the solar wind produces several TB of data each time step. Space and solar missions provide increasingly massive dat sets as well. Human investigation or even traditional automatic methods struggle to deal with this size and complexity. Recently machine learning (ML) has become the focus of concentrated attention in our community. AIDA is an example of a community-building project to address practical problems in this area.
With the tools of AIDA we provide methods to study with compatible integrated methods, based on python, both results from observations and from simulation.
We will present the methods developed by AIDA, focusing on machine learning (ML) methods to analyse particle distributions, to analyse time series, and too analyse images (including higher dimensional data sets). We will show both supervised and unsupervised methods to identify extreme events such as reconnection. We will show the application to both simulation results and observational data.
Fast magnetic reconnection plays a fundamental role in driving explosive dynamics and heating in the solar chromosphere. The reconnection time scale of traditional models is shortened by the onset of the coalescence instability, which forms a turbulent reconnecting current sheet through plasmoid interaction. Non-equilibrium ionisation–recombination processes can significantly alter the time scale of magnetic reconnection by changing the plasma composition, therefore it is essential to evaluate their contribution in the development of plasmoid coalescence. In this talk I investigate the role of ionisation and recombination in the development of fast magnetic reconnection in a partially ionised plasma through the study of the coalescence instability of plasmoids. Unlike the processes occurring in fully ionised coronal plasmas, relatively little is known about how fast reconnection develops in partially ionised plasmas (PIPs) of the chromosphere. I will present 1D and 2.5D preliminary simulations of a two-fluid model of a partially ionised plasma (PIP) and show how the dynamics change in the presence and absence of ionisation and recombination processes. In our 1D calculations, as the current sheet collapses, it drives a burst of ionisation. This results in the current of the current sheet growing at a slower rate than calculations without ionisation and recombination, and in a thicker current sheet. I will discuss the consequences of ionisation and recombination on chromospheric plasmas, based on our 2.5D simulations.
Coronal forbidden lines in the visible and near infrared (NIR) provide a range of plasma diagnostics to probe the solar corona.
They have not been explored much, but this is changing, with several facilities coming into operation, primarily DKIST.
We briefly review the importance of accurate atomic rates and proper modelling for these forbidden lines.
We provide examples of new calculations for a few ions which are being made available via the CHIANTI database.
We then present the results of two eclipse observations, in 2017 and 2019, where we have combined NIR AIR-Spec observations with EUV observations by Hinode EIS. AIR-Spec is a pathway mission for DKIST: a NIR spectrometer designed to observe eclipses from an aircraft flying at an altitude of 14 km. We have obtained new measurements of temperatures, densities from line ratios, and elemental abundances. These plasma parameters are in overall agreement with our previous results. Most notably, that the quiet corona has a sulphur abundance close to the photospheric one.
The passage of comets in the solar corona can be a powerful tool to probe the local plasma properties. One such case is offered by Comet Lovejoy, which gives us the possibility to infer the coronal plasma density along the magnetic field lines intersected by the comet trajectory, thanks to the emission by cometary ions injected along the magnetic field, forming so-called striae.
Here, we carry out a preliminary study of these striae, as observed by the Atmospheric Imaging Assembly (AIA) aboard the Solar Dynamics Observatory (SDO) during the ingress phase of the comet orbit. We consider the images in the 171 Å line, where emission from oxygen ions O$^{4+}$ and O$^{5+}$ is found.
The striae are described as due to the beam of oxygen ions along the local magnetic field, with the injection beam velocity decaying because of collisions. Also, ion collisional diffusion contributes to ion propagation. Both the collision time for velocity decay and the diffusion coefficient depend on the ambient plasma density so that measurements of the striae length can be related to the local density. A probabilistic description of the ion beam density along the magnetic field is developed, where the beam position is given by the velocity decay and the spreading of diffusing ions is described by a Gaussian probability distribution. Profiles of emission intensity along the magnetic field are computed and compared with the profiles along the striae observed by AIA, in order to estimate the ambient plasma density.
Shock waves driven by Coronal mass ejections (CMEs) can accelerate particles. Radio signatures of electron beams accelerated at the shock front (type II bursts) are produced when the shock wave propagates through the solar atmosphere. Ground-based radio observations allow us to study shock waves in the low corona while space-based radio observations provide us the opportunity to track shock waves in the inner heliosphere.
The preferable location of the type II radio sources on the surface of the shock wave has been a long-discussed question. We address this question in the study of a shock wave associated with a flare/CME event and complex radio event on September 27, 2012. We employ a novel approach, combining the results from the radio triangulation analysis with shock wave modelling.
We first reconstruct the shock wave in 3D space using multi-viewpoint white light observations by SDO and STEREO spacecraft, and then model the evolution of the shock wave using a 3D MHD background coronal model produced by the MAS (Magnetohydrodynamics Around a Sphere Thermodynamic) model.
We first analyze the global evolution of the wave parameters and then localize the areas which could be the source regions of radio emission. We study the temporal evolution of the upstream plasma characteristics and the shock wave parameters. Our results indicate a complex relationship between the different shock wave parameters. However, the shock wave geometry and its relationship with the shock strength seem to play the most important role in the generation of type II radio emission.
The Bent Crystal Spectrometer (BCS) observed high resolution spectra of flares between 1980 and 1989. The instument's channel 1 recorded the triplet of lines arising from He-like Ca (Ca XIX) together with several satellite lines formed from doubly excited states of the Ca XVIII ion. Portions of the continuum emitted by flares were also observed, free from instrumental effects (crystal fluorescence). A collimator in front of the BCS allowed only emission from particular active regions, so preventing overlapping of spectra from multiple active regions. The SMM BCS spectra are still the best ever recorded for flaring hot plasmas. Early analysis of these Ca spectra revealed changing abundances of Ca between flares for ~146 events observed early in the Mission. In the present study, we extended this study for the spectra obtained over the entire SMM Mission duration using updated instrument response data. We determined/redetermined the absolute (relative to hydrogen) abundances for 207 flares during their decay phases with a precision of 1 to 3 % for some flares, the best abundance determinations for any coronal sources. We describe the new data reduction process and compare derived flare abundances with other selected flare characteristics as well as average calcium abundances determined from other measurements.
During April, 2019, several groups of type III radio bursts were observed, starting from the metric wavelength range (ground based observations) and continuing in the hectometric to kilometric range (space based observations). A majority of the type III bursts was observed by LOFAR (Low Frequency Array), by radio instruments on Stereo A and Wind spacecraft, and also by the Parker Solar Probe (PSP).
We focus this study on a small group of type III bursts observed on April 03, in the time window from 16:40 UT until 17:00 UT. The aim of the study is to map the propagation of the type III bursts and compare the obtained plasma densities with the density profiles provided by EUHFORIA (EUropean Heliospheric FORecasting Information Asset) model, and with in-situ observations from PSP which was located in a close proximity. First results indicate that the type III bursts do not follow, as generally considered, Parker spiral but they propagate strongly southward from their source region. It is possible that this unusual propagation path is induced by the weak CME that preceded the radio bursts and disturbed the ambient solar conditions.
We hereby present the interferometric LOFAR observations of the solar radio event on 22 August 2017, during which the type III radio bursts have been detected. Solar radio image and dynamic spectra were recorded in the 10 – 90 MHz frequency band. Additionally to LOFAR observations, the data recorded by instruments onboard the Solar Dynamics Observatory (SDO) in the UV spectral range, GOES and RHESSI in X-ray spectral range complement observations in the radio field. Our study shows that the interferometric LOFAR observations, in combination with observations at other wavelengths can give better understanding of the environment in which the type III radio events occur.
The atmospheric conditions of the Sun are encoded within the line emission of different atomic transitions (spectra). To infer the physics of the solar atmosphere from spectra, we have to compare these observations with synthetic outputs from simulations. It is however often the case that the thermodynamic solutions satisfying an observation are degenerate, with different variations of vertically stratified temperatures, densities, and velocity fields leading to the same synthetic output. It is therefore desirable to restrain the solution space of our simulations by analyzing multiple spectral lines simultaneously. We use machine learning methods in combination with observations from the Interface Region Imaging Spectrograph (IRIS), to calculate the entire set of possible spectral responses over all spectral windows during a solar flare giving a single fixed Mg II spectrum. The results provide us with an automatic way of analyzing the Sun through a multithermal lens and provide us with a rich set of constraints for simulations and interpretations. This method helps shed light on the emission found at the edge of flare ribbons, showing central reversals in chromospheric and transition region lines, as well as deep atmospheric heating as indicated by enhanced Fe II emission.
AB Dor is an active rapidly rotating K0 dwarf which rotates $\sim$ 50 times faster than the Sun. We have studied flare light curves from AB Dor using the archival observations from the XMM-Newton satellite and detected quasi-periodic pulsations (QPPs). Periods and damping times of QPPs are derived and compared to those for solar and other stellar flares. These parameters are generally found to be larger than those from the solar and other stellar QPPs. Kolmogorov-Smirnov (K-S) test reveals that the QPPs found in the post-flare light curves of AB Dor are similar to the previously reported solar and stellar QPPs. The scaling law of damping period with oscillation time of flare generated QPPs interestingly exhibit the same nature as observed in the flares at the Sun and other magnetically active solar-type stars. This implies that QPPs at AB Dor may have a similar origin as in the Sun and other active stars. Thus the physical origin can be attributed due to the magnetoacoustic modes. To the best of our knowledge, the present findings are the first evidence of the wave-generated QPPs observed at AB Dor, and we discuss its physical implications in its stellar coronae.
We present observations of an M class flare with the LOw Frequency ARray (LOFAR) in the moring hours of 7 September 2017. The flare was accompanied by strong type III radio bursts. LOFAR interferometric images in the low band frequency range of 20 - 80 MHz show distinct sources that show variations in their positions, and intermittent dual source structures. We identify these as fundamental and harmonic emission, with the one or other being dominant at times. These distinct sources and their evolution allow for obtaining separate lightcurves for both fundamental and harmonic emission.
The data show that transport effects due to refraction and scattering play a significant role, both in source separation and drift of their apparent positions. Comparing the light curves of fundamental and harmonic pairs, e.g. 35 MHz fundamental and 70 MHz harmonic, enables studies of radio wave propagation in the solar corona. Observations of harmonic emission can provide information on source locations high in the corona, where fundamental emission would be near or below the ionospheric cutoff at 10 MHz. These are relevant for the transition into the solar wind, and for joint observing campaigns with Parker Solar Probe and Solar Orbiter that are currently investigating the inner heliosphere.
The Sun produces highly dynamic and eruptive events that can drive shocks through the corona. These shocks can accelerate electrons, which result in plasma emission in the form of a type II radio burst. Despite the large number of type II radio bursts observations, the precise origin of coronal shocks is still subject to investigation. Here we present a well observed solar eruptive event that occurred on 16 October 2015, focusing on a jet observed in the extreme ultraviolet (EUV) by the Atmospheric Imaging Assembly (SDO/AIA), a streamer observed in white-light by the Large Angle and Spectrometric Coronagraph (SOHO/LASCO), and a metric type II radio burst observed by the LOw Frequency Array (LOFAR). LOFAR interferometrically imaged the fundamental and harmonic sources of a type II radio burst and revealed that the sources did not appear to be co-spatial, as would be expected from the plasma emission mechanism. We correct for the separation between the fundamental and harmonic using a model which accounts for scattering of radio waves by electron density fluctuations in a turbulent plasma. This allows us to show the type II radio sources were located ∼0.5 R⊙ above the jet and propagated at a speed of ∼1000 kms−1, which was significantly faster than the jet speed of ∼200 kms−1. This suggests that the type II burst was generated by a piston shock driven by the jet in the low corona.
Solar radio spikes are short duration and narrow bandwidth fine structures in dynamic spectra observed from tens of MHz to the GHz range. Their very short duration (10-1000 s) and narrowband emission is indicative of the possibly fastest small-scale energy release processes observed in the solar corona, yet the origin of the spikes is not established. We present, for the first time, spatially, frequency and time resolved observations of individual radio spikes associated with an eruptive solar flare-CME event using the LOw Frequency ARray (LOFAR). The spikes present low frequency drift rates, yet imaging spectroscopy of individual spikes between 30-45 MHz show apparent superluminal spike source motions. Comparison of spike characteristics with that of individual Type IIIb striae show similarities in duration, bandwidth, drift rate, and apparent areal increase, as well as the apparent motion in the image plane. The observed spatial, spectral, and temporal properties of the spike bursts are consistent with plasma radio emission escaping through anisotropic scattering density turbulence that induces the shift in the apparent source location over time.
Plasma turbulence can be viewed as a magnetic landscape populated by large- and small-scale coherent structures, consisting notionally of magnetic flux tubes and their boundaries. Such structures exist over a wide range of scales and exhibit diverse morphology and plasma properties. Interactions of particles with turbulence may involve temporary trapping in, as well as exclusion from, certain regions of space; generally controlled by the topology and connectivity of the magnetic field. In some cases, such as SEP ``dropouts'', the influence of the magnetic structure is dramatic; in other cases, it is more subtle, as in edge effects in SEP confinement. With Parker Solar Probe now closer to the sun than any previous mission, novel opportunities are available for examination of the relationship between magnetic flux structures and energetic particle populations.
We present a synergistic use of the magnetic helicity-partial variance of increments (PVI) technique paired with IS$\odot$IS observations of energetic particles (EPs). The filtered magnetic helicity detects large-scale helical flux tubes while the PVI identifies their boundaries, thus giving a multi-scale finer description of the structures. The correlation with EP fluxes show direct observational evidence of the modulation provided by flux tubes.
We find that helical flux tubes, accompanied by bounding large-PVI patches, act as hard boundaries that inhibit EP transport either confining populations within the helical field, or excluding them from entering it.
Solar electrons beams are accelerated in the corona, into the solar wind and beyond in the Solar system through eruptive mechanisms at the surface of the Sun such as flares. These beams of non-thermal electrons evolve as a function of distance from the Sun, interacting with the background plasma and growing Langmuir waves as they propagate. Subsequent radio and X-ray wavelength emission is also seen. Insight into electron beam transport effects allows us to disentangle them from the acceleration properties and provides a framework for using in situ measurements to diagnose coronal acceleration characteristics. Through beam-plasma structure simulations we study the interactions between these electron beams and the background plasma of the solar corona and beyond at different distances from the Sun. This allows us to determine what is the maximum electron velocity responsible for Langmuir wave production and growth, and consequently which electron energies these correspond to. Understanding the mechanisms driving the change in the maximum electron velocity will permit more accurate predictions in electron onset as well as arrival times, relevant for space weather applications and the understanding of the subsequent emissions at radio and X-ray wavelength. Moreover, our radial predictions can be tested against in-situ electron and plasma measurements from the instruments on-board the Solar Orbiter and Parker Solar Probe spacecrafts.
This contribution focus on the analysis of the distribution function of different physical magnitudes of the solar wind. The data set comes from the ACE spacecraft located at the L1 point and covers almost two solar cycles, from 1998 to 2017.
We propose a bi-Gaussian distribution, formed by the addition of two Gaussian distribution functions, to characterize the solar wind. Each Gaussian function corresponds to the contribution of one of the different regimes of the bulk solar wind: fast and slow wind.
We apply this approach not only to the proton speed, but also for the interplanetary magnetic field magnitude, proton temperature and proton density, and we obtain a bimodal distribution which allow us to characterize each regime of the bulk solar wind.
Our results also show a clear correlation between some fitting parameters and the solar cycle.
We also apply the Bi-gaussian approach to the solar wind composition, more precisely to the average iron charge state. From these results we are able to identify interplanetary coronal mass ejections which were not included in previous catalogues.
High-energy particles penetrate spacecraft and to a different extent affect the performance of instruments flown on board space missions. Consequently, spacecraft carry particle detectors for both diagnostics and scientific purposes that allow to monitor the galactic cosmic-ray and solar energetic particle fluxes during the whole mission elapsed time. These data allow us to disentangle long and short-term variations of the GCR flux associated with the solar activity, the passage of interplanetary counterparts of coronal mass ejections and high speed solar wind streams. Monte Carlo simulations of the GCR tracks observed in the Metis coronagraph visible light images have shown that the background of spurious pixels fired by cosmic rays is only a fraction of the order of 10-4 of the whole pixel sample and therefore they do not affect sensibly the quality of the Metis images. Moreover, the comparison of the simulations with the cosmic-ray matrices obtained from the Metis VL light images mainly consisting of primary and secondary particles generated by primary protons indicate that Metis may play the role of a detector to study the variations of GCRs and SEPs during the next decade.
Coronal Mass Ejections (CMEs) are some of the most energetic solar events that expel plasma and magnetic field into the interplanetary medium. Stealth CMEs represent a special type of solar eruptions that, in most cases, can be clearly seen in coronagraph observations, but lack distinct source signatures. We simulate consecutive CMEs ejected from the southernmost part of an initial configuration constituted by three magnetic arcades embedded in a globally bipolar magnetic field. The first eruption is driven through shearing motions at the solar surface. The following eruption is either a stealth blob-like CME, resulting from the reconnection of the coronal magnetic field, or another shearing driven flux rope. All CMEs are expelled into a bimodal solar wind.
We analyse the parameters that contribute to the occurrence of the second CME, as well as its influence onto the first eruption during the propagation to 1AU by simulating also a single erupting flux rope.
We track the two double-CME cases until Mercury and 1AU, and compare their simulated signatures with the in-situ data of a similar multiple CME event that occurred between 21-22 Sept. 2009, obtaining a good correlation.
Furthermore, we impose the same shearing speeds along the polarity inversion line of the southern arcade, but immersed into a faster solar wind, to analyze the effect of the overall magnetic structure and of the wind onto the resulting eruptions, propagation and geoeffectiveness. The latter is studied via the Dst index, computed using an empirical model from the simulated parameters of the ICMEs.
The observations of the resonantly scattered ultraviolet emission of the coronal plasma obtained with UVCS-SOHO, properly designed to measure the wind outflow speed by applying the Doppler dimming diagnostics, noticeably fostered the investigation of the wind in the inner solar corona. Metis on Solar Orbiter complements the UVCS spectroscopic observations, by simultaneously imaging the polarized visible light and the \ion{H}{i}~Lyman-$\alpha$ corona in order to obtain high spatial and temporal resolution maps of the outward velocity of the continuously expanding solar atmosphere. The polarized visible light (580-640~nm), and the ultraviolet \ion{H}{i}~Ly$\alpha$ (121.6~nm) coronal emissions, obtained in the two Metis channels, are combined in order to measure the Doppler dimming of the UV emission, relative to a static corona. The plasma outflow velocity is then derived as a function of the measured Doppler dimming. The Metis first light observations, obtained on May 15, 2020, near the end of the commissioning phase of the Solar Orbiter mission, provide the first instantaneous image of the speed of the plasma outflows in the corona during the minimum of solar activity, from 4~$R_\odot$ to 6~$R_\odot$, and allow us to identify the layers where the fast and slow wind flow is observed.
Both coronal holes and active regions are source regions of the solar wind. The distribution of these coronal structures across both space and time is well known, but it is unclear how much each source contributes to the solar wind.
We have used photospheric magnetic field maps from the past four solar cycles to estimate what fraction of magnetic open solar flux is rooted in active regions, a proxy for the fraction of all solar wind originating in active regions. The fractional contribution of active regions to the solar wind varies between 30% to 80% at any one time during solar maximum and is negligible at solar minimum, showing a strong correlation with sunspot number. While active regions are typically confined to latitudes $\pm$30$^{\circ}$ in the corona, the solar wind they produce can reach latitudes up to $\pm$60$^{\circ}$. Their fractional contribution to the solar wind is also highly variable, changing by $\pm$20% on monthly timescales within individual solar maxima.
These results quantify the importance of active regions as solar wind sources, providing motivation for understanding active region solar wind heating and acceleration using Parker Solar Probe and Solar Orbiter during solar cycle 25.
Interest in predicting space weather conditions constantly pushes the advance of state-of-the-art three-dimensional(3D) magnetohydrodynamic (MHD) models of the solar corona and the solar wind, which need to be validated with observational data. Tomography of the solar corona is the only observational technique that can currently provide empirical data of the solar atmosphere in a 3D global fashion. In this work we carry out a validation study of the latest version of the Alfvén Wave Solar atmosphere Model (AWSoM), comparing its results with tomographic reconstructions of physical parameters of the solar corona. For this anlysis, we select rotations from the recent deep minimum of solar activity, between solar cycles 24 and 25, which renews the opportunity to study the Sun-Earth connection under the simplest solar and space environment conditions. Based on narrow band EUV coronal images provided by the SDO/AIA instrument, we carry out tomographic 3D reconstruction of the coronal electron density and temperature in the range of heliocentric heights $r \le 1.25~{\rm R}_\odot$. Based on polarized visible brightness (pB) coronagraph images provided by the SoHO/LASCO-C2 instrument, we carry out tomographic 3D reconstruction of the coronal electron density in the range of heliocentric heights $\approx 2.5 - 6.0~{\rm R}_\odot$. We compare the MHD model with the tomographic reconstructions in their respective range of heights and discuss the current capability of the AWSoM model to reproduce the reconstructions in specific coronal magnetic structures.
We perform hydrodynamic 2D simulations of solar convection. We aim to study the dependence of different physical parameters, the box size, and box aspect ratio on the actual convective motions we observe in the numerical model. Furthermore, we need to evaluate the performance of different Input/Output strategies on supercomputers, in order to plan and run future large-scale magneto-hydrodynamic models of the solar atmosphere. To this end, we use our convection model for a performance analysis of different numerical IO schemes. We use a large simulation domain together with a high grid resolution in order to provide high Reynolds numbers in the numerical model. This allows us to model the solar convection zone down to 20 Mm below the surface and include the solar atmosphere up to 10 Mm. We use 1024x256 grid points with initial conditions matching the gravity, temperature, and density stratification of the Sun. After the bottom of the box is heated sufficiently, the convective motions set in and transports energy towards the surface. At the top of the convection zone, material is ejected into the atmosphere, before falling down again.
We conclude that we require a minimum horizontal extent of the simulation domain and a minimum box aspect ratio, in order to obtain realistic convection cells. Also we find that HDF5 output is required for future large-scale computer models, because the traditional IO strategy of the Pencil Code puts too high demands on nowadays supercomputer file systems, both in storage space requirements and number of file operations.
The poster presents observations of variability of the emission cores of Mg II k & h lines in the solar cycle 24 and their center-to-limb variations acquired by the Interface Region Imaging Spectrograph (IRIS) in the years 2013-2020. We use 91 full-disk NUV IRIS mosaics covering the raising phase, maximum, decline, and the end of the solar cycle 24. For this analysis, the solar disk is divided into ten concentric equiareal zones. Data averaged over the zones represent the center-to-limb variation of the Mg II k & h line cores. The time series of IRIS spectral irradiance correlates well with the UV indices (Bremen Composite Magnesium II Index and the Composite Solar Lyman-alpha Index) with the correlation coefficients of 0.90 - 0.94, thus verifying the long-term stability of IRIS radiometric calibration. The Mg II k & h emission cores show significant center-to-limb variation. Their wavelength-integrated intensities decrease toward the limb suggesting overall limb darkening. However, broadening of the emission cores toward the limb invokes the limb brightening in narrow wavelength intervals where the intensities are higher than in the disk center. The time series of calibrated full-disk IRIS mosaics allows also to answer a question whether the quiet areas of the solar atmosphere change over the solar cycle 24 at chromospheric layers.
Weak magnetic field elements make a dominant contribution to the total magnetic field on the solar surface. Still, quite little is known of their properties and long-term occurrence.
We study the spatial-temporal evolution of the weak-field shift and skewness of the distribution of photospheric magnetic field values during solar cycles 21-24. We use WSO and SOLIS/VSM synoptic maps to construct butterfly diagrams for weak-field shifts and skewness.
Weak-field shift and full-field skewness depict a spatial-temporal solar cycle evolution, which is closely similar to that of the large-scale surface magnetic field. Magnetic field distribution has a systematic non-zero weak-field shift and a large skewness already at the emergence of active regions. We find evidence for coalescence of opposite-polarity fields during the surge evolution. This is clearly most effective at the supergranulation scale. However, a similar dependence of magnetic field coalescence on spatial resolution was not found in polar coronal holes.
Our results give evidence for the preference of even the weakest field elements toward prevailing magnetic polarity since the emergence of active regions, and for a systematic coalescence of stronger magnetic fields of opposite polarities to produce weak fields during surge evolution and at the poles. Our results suggest that supergranulation process is reduced or inhibited in polar coronal holes. This result is further supported, e.g., by the fact that the spectral index of diffusion of coronal bright points is larger in the polar coronal hole than at other latitudes, indicating that diffusion is less limited in the polar coronal hole.
Since the release of the first TESS sector the possibility of examining stellar flares and stellar dynamo compared to the solar dynamo and solar flares has increased. Thanks to this observations we tried to estimate staining of low mass stars with visible variability of their luminosity. We managed to do this using newly created software called BASSMAN (Best rAndom StarSpots Model calculAtioN) that allows to estimate amount of spots on star and parameters of the estimated spots. Trying to recreate spots on star can help examine more deeply how inner structure of the star can be connected to staining of star, how the spots evolve or appear on the star or how spots are related to flares. Here I will present results of modelling of star spots for 2 stars with our new tool and compare the results with the previous reconstructions of the spatial distribution of spots.
Here we present the concept feasibility study of the Galileo Solar Space Telescope Mission (GSST Mission) proposed by the Brazilian National Institute for Space Research (INPE). The study was conducted at the Space Missions Integrated Design Center (CPRIME - Centro de Projeto Integrado de Missões Espaciais). The GSST shall contribute to the understanding of the evolution of the magnetic structure of the Sun and its influence on the Earth's space environment. The requirements proposed for the mission include high spatial and temporal resolution observations. Those measurements involve observations of the photosphere and outer layers of the solar atmosphere, observations of the variability of TSI, and in situ observations. The study included: (a) the definition of the scientific objectives; (b) the identification of the system drivers; (c) the definition of the candidate solutions for the system; (d) the conceptual design of the mission’s architecture components, including the optical payloads; (e) the pointing accuracy analysis of the designed attitude control subsystem; (f) the simulation and verification of the mission operational concept; (g) the assessment of the ground segment required to fulfill the mission; (h) estimate of the schedule for the development of the mission; and (i) the risk analysis. The optical payload architecture, orbit, and ground segment were identified as the main system drivers. The concept of two full disk telescopes and one high-resolution telescope for visible and ultraviolet spectropolarimetric observations have been the basis for the solution of the optical payload architecture selected for scientific purposes. INPE's GSST Mission Working Group.
The presence of elongated magnetic polarities in active-region (AR) line-of-sight (LOS) magnetograms indicates the existence of twist in the flux tubes forming them. These elongations, a.k.a. magnetic tongues, which are mostly visible during the emergence phase of ARs, determine the magnetic field distribution observed in LOS magnetograms, and therefore, affect the measurement of AR characteristics such as their tilt angles. Obtaining a good estimation of tilt angle evolutions and spatial variations plays a key role in constraining flux-transport dynamo models, as Joy's law is fundamental for the formation and evolution of the polar field. In this work we aim to estimate the intrinsic geometrical properties of the twisted flux tubes, or flux ropes (FRs), that form ARs by comparing observed LOS magnetograms with synthetic magnetograms derived from a toroidal magnetic flux tube model. Analyzing a sequence of 66 magnetograms, corresponding to the emergence of NOAA AR 10268, we model the evolution of parameters such as the tilt angle, the length and cross-section size of the FR, and the emergence rate assuming a kinematic rise of the torus. Our method uses a probabilistic scheme based on the Bayes theorem to infer the most probable intrinsic parameters of the emerging flux tube, assuming a normal distribution for the differences between the model and the observations. We discuss the importance of the prior distribution for all the model parameters in order to avoid degeneracies of the optimal solution. We also propose a recursive method to constrain these priors directly from the observations.
Today’s picture of the internal solar rotation rate profile results essentially from helioseismic analyses of frequency splittings of resonant acoustic waves. This has the limitation that the rotation profile is an average over the northern and southern hemispheres.
Here we present another, complementary estimation of the internal solar rotation rate using the perturbation of the shape of the acoustic waves. For this purpose, we extend the global helioseismic approach developed previously for the investigation of the meridional flow to work on the
components of the differential rotation. We find that the
rotation rate profiles from the two different approaches are qualitatively in good agreement, while the new measurements provide the asymmetric rotation components in addition.
Active Regions (ARs) in their emergence phase are known to be more flare productive and eruptive than ARs in their decay phase. In this work, we focus on complex emerging ARs composed of multiple bipoles. Due to the compact clustering of the different emerging bipoles within such complex multipolar ARs, collision and shearing between opposite non-conjugated polarities produce “collisional polarity inversion lines” (cPILs) and drive rapid photospheric cancellation of magnetic flux. The strength and the duration of the collision, shearing, and cancellation are defined by the natural separation of the conjugated polarities during the emergence phase of each bipole in the AR. This mechanism is called “collisional shearing”. In Chintzoglou et al (2019), collisional shearing was demonstrated using two emerging flare- and CME-productive ARs (NOAA AR11158 and AR12017) by measuring significant amounts of magnetic flux canceling at the cPIL. This finding supported the formation and energization of magnetic flux ropes before their eruption as CMEs and the associated flare activity.
Here, we provide results from data-driven 3D modeling of the coronal magnetic field, capturing the recurrent formation and eruption of energized structures in support of the collisional shearing process. We discuss our results in relation to flare and eruptive activity.
Spectropolarimetric reconstructions of the photospheric vector magnetic field are intrinsically limited by the so-called 180$^\circ$ ambiguity in the orientation of the transverse component. The successful launch and operation of Solar Orbiter has made the removal of the 180$^\circ$-ambiguity possible using solely observations obtained from two different vantage points. While the exploitation of such a possibility is straightforward in principle, it is less so in practice and it is therefore important to assess the accuracy and limitations, as a function of both the satellites orbits and measurement principles. In this work we present a stereoscopic disambiguation method (SDM) and discuss a thorough testing of its accuracy in applications to modeled active regions and quiet Sun observations. The SDM is proven to to reach a 100% disambiguation accuracy when applied to moderately-to-well resolved fields. In such favourable conditions, the accuracy is almost independent of the satellites relative position, with the obvious exceptions of configurations where the satellites are within few degrees from co-alignment or quadrature. Even in the case of disambiguation of quiet Sun magnetograms with significant under-resolved scale, the SDM provides an accuracy between 82% and 98% depending on the field strength. Additionally, we provide an example of the expected accuracy as a function of time that can be used to optimally place remote-sensing windows during Solar Orbiter observation planning. Finally, a preliminary discussion of the effect of the viewing angle on the observed field as modeled by Solar Orbiter instrument simulations is presented.
The solar photosphere and the outer layer of the Sun's interior are characterized by convective motions, which display a chaotic and turbulent character. In order to further investigate those motions, we estimated the pseudo-Lyapunov exponents of the overshooting convection described by current state-of-the-art observations of the Sun’s surface. In particular, we applied a method employed in the literature to estimate the pseudo-Lyapunov exponents, as well as another technique deduced from their definition, to the spectro-polarimetric data acquired with the ground-based Interferometric Bidimensional Spectrometer (IBIS) and Crisp Imaging SpectroPolarimeter (CRISP) instruments, and the space-borne Helioseismic and Magnetic Imager (HMI). Following previous studies in the literature, we computed maps of four quantities which were representative of the physical properties of solar plasma in each observation, and estimated the pseudo-Lyapunov exponents from the residuals between the values of the quantities computed at any point in the map and the mean of values over the whole map. We found that all the computed exponents hold negative values, which are typical of a dissipative regime, in contrast to previous results reported in the literature. We also found that the values of the estimated exponents increase with the spatial resolution of the data and are almost unaffected by small concentrations of magnetic field.
We studied physical properties of the magnetic field above the sunspot which was observed on September 10, 2014 near the center of the solar disk during the time period 16:20-18:20 UT by the SDO/AIA/HMI and IRIS instruments. We detected a magnetic field flux tube above a sunspot umbra where vertical magnetic field lines formed a connection between the inner layers of the solar atmosphere and the solar corona. We studied a mechanism of MHD waves transfer from the photosphere without dissipation or reflection before reaching the corona. We also discuss a significance of such events in terms of the possible propagation and scattering of magnetic energy in the Sun's atmosphere, including solar corona. We can explain how the magnetic field flux tubes connecting the individual atmospheric layers can distribute the photospheric and chromospheric magnetic field energy across the active region. This mechanism can contribute to the coronal energy balance and improve our knowledge how the coronal heating is maintained.
Observations of the Sun with the Atacama Large Millimeter/sub-millimeter Array (ALMA) facilitate chromospheric studies at high spatial and temporal resolution.
We strive to evaluate observational data and determine the origin of the detected small-scale structures with the support of numerical simulations.
For this purpose, high-cadence Bifrost 3D simulations and radiative transfer calculations are used to construct brightness temperature maps at wavelengths corresponding to the spectral bands of ALMA.
A detailed study of shock waves in the simulation is made to characterise the corresponding signatures at mm-wavelengths.
Several hundred small-scale dynamic features are detected in the (~40 min) observation, which agrees well with shock wave signatures.
The ALMA bands effectively trace shock waves through the chromosphere. It is shown by degrading the resolution of the mm-maps, to what degree the dynamic signatures are expected to be observable, at different wavelengths and spatial resolutions. The specific spatial scales and contrasts, together with the size and shape of the effective resolution element, are very important for how the dynamic signatures are perceived.
In addition, the formation heights of the mm-wavelength radiation in connection to the small-scale dynamics is investigated and it is shown that the slope of brightness temperature within a receiver band can be used to give an estimation of the slope of the local gas temperature at the sampled layers and provides a better understanding of the underlying physical conditions of the dynamic features.
We present a unique set of observations of a confined minifilament eruption from the quiet-Sun during solar minimum. The Nuclear Spectroscopic Telescope Array (NuSTAR) spotted a tiny, compact hard X-ray (HXR) flare on 2019 April 26, peaking about 02:06UT lasting for a few minutes, finding brief emission >5MK. Observations with SDO/AIA and Hinode/XRT show this HXR emission was due to a tiny flare arcade underneath a confined minifilament eruption – behaviour similar to those seen in both major active-region filament eruptions and minifilament eruptions that lead to coronal jets. This eruption occurred near disk-centre, so the Earth orbiting observatories provide a top-down view of the event, but fortuitously a side-on view is obtained from STEREO-A/SECCHI, giving a clearer sense of eruption geometry. Line-of-sight magnetograms from SDO/HMI show that this eruption is due to opposite polarity flux moving together and cancelling and not due to flux emergence. We also explore the possibility of non-thermal emission due to accelerated electrons from the HXR observations of this tiny quiet Sun impulsive energy release.
ALMA provides a new set of eyes to look at the stars including our Sun. In particular, the brightness temperatures provided by ALMA give insights about the thermal structure and activity of stellar atmospheres. The Sun, being the closest star, can be observed well resolved and thus be used as a reference case for solar-like stars. The overall aim of the presented study is to construct more robust solar/stellar activity indicators using ALMA observations in comparison with classical diagnostics.
Here, full disk solar maps from ALMA are compared with SDO-AIA and HMI maps and, with full disk H-alpha and Ca II maps to understand the correlation between them, which also provides constraints for the height range from where these mm emissions originate. The centre to limb variation in temperature observed for ALMA maps shows limb brightening which confirms the expectation that the radiation observed with ALMA originates from the chromosphere. In order to transfer the insights gained from solar ALMA observations to other stars, the full disk solar maps are converted into a corresponding stellar signal. Here we present the first results.
In this paper, the phenomenon of vortex shedding around a circular cylindrical obstacle is studied numerically in magnetohydrodynamic (MHD) conditions in three spatial dimensions using the numerical code Lare3d. A parametric study was performed for different values of magnetic field perpendicular to the plasma flow plane. This model mimics coronal mass ejection flowing around a coronal loop, which is known as a probable mechanism for excitation of kink-mode oscillations in coronal loops. The phenomenon of vortex shedding has been widely studied in hydrodynamic conditions in both science and engineering, it has also been investigated by a number of numerical simulations in magnetic field environments, mainly in two dimensions. In MHD conditions, however, it is poorly understood.
Based on simultaneous spectroscopic measurements in the H$\alpha$ line and the Mg II k & h lines, Guiping et al. (2019) arrived at two solutions by comparing the observed and synthetic parameters of the H$\alpha$ line with 1D non-LTE modeling. They obtained relatively high temperatures at a microturbulent velocity of 8 km/s, while the temperatures at 16 km/s were standard values. Here we want to investigate the behavior of this prominence in more detail. We analyze both the H$\alpha$ line and the two Mg II lines detected by IRIS and compare the observed and synthetic profiles for all lines using five different spectral parameters. The analysis is based on spectral inversions using an extended grid of prominence 1D slab models. Preliminary results will be presented together with 2D maps of various physical parameters, and we will discuss our best-fit solutions with respect to the radiative-equilibrium models.
Spectroscopic observations of the emission lines formed in the transition region (TR) commonly show persistent downflows of the order of 10--15 kms$^{-1}$. Their cause, however, is still not fully clear and has remained a matter of debate.
Using two sets of coordinated data from SST, IRIS, and SDO, we aim to understand the cause of such downflows by studying the coronal and TR responses to the recently reported chromospheric downflowing rapid red-shifted excursions (RREs), and their impact on solar atmospheric heating. To provide theoretical support, we use an already existing 2.5D magnetohydrodynamic simulation of spicules performed with the Bifrost code.
We show several examples of the spatio-temporal evolution of downflowing RREs across multiple channels, ranging from the cooler chromosphere to the hotter corona. Our analysis suggests that they are likely the returning components of the previously heated spicular plasma. Furthermore, the TR Doppler shifts associated with them are close to the average redshifts observed in this region, which implies that they could (partly) be responsible for the persistent downflows observed in the TR. We also propose two mechanisms (an upflow followed by a downflow and downflows along a loop), from the numerical simulation, that could explain the ubiquity of such downflows. A detailed comparison between the synthetic and observed spectra, reveals a distinctive match, and further suggests an impact on the heating of the solar atmosphere.
We present compelling evidence that suggests that many of the downflowing RREs are the chromospheric counterparts of the TR and lower coronal downflows.
The emission in the near ultraviolet Ca II H & K lines, often quantified via the S-index, has been serving as a prime proxy of solar and stellar magnetic activity. Despite the broad usage of the S-index, the link between coverage of a stellar disk by magnetic features and Ca II H & K emission is not fully understood. In order to fill this gap we developed a physics-based model to calculate the solar S-index. To this end, we used the distributions of the solar magnetic features derived from simulations of magnetic flux emergence and surface transport, together with the Ca II H & K spectra synthesised using a non-LTE radiative transfer code.
We show that the solar S-index value is influenced by the inclination angle between the solar rotation axis and the observer’s line-of-sight, i.e. the solar S-index values obtained by an out-of-ecliptic observer are different from those obtained by an ecliptic-bound observer. This is important for comparing the magnetic activity of the Sun to other stars. We computed time series of the S-index as they would be observed at various inclinations dating back to 1700. We find that depending on the inclination and period of observations, the activity cycle in solar S-index can appear weaker or stronger than in stars with a solar-like level of magnetic activity. We show that there is nothing unusual about the solar chromospheric emission variations in the context of stars with near-solar magnetic activity.
The Atmospheric Imaging Assembly (AIA) on the Solar Dynamics Observatory (SDO) is one of the most-used data sources in solar physics. Its point spread functions (PSF) were well calibrated by the instrument team, and allows high-quality observations of the solar corona at a resolution of ~1.5 arcsec for quiet Sun and active regions. However, it is suspected that low-emission features such as coronal holes still contain a significant contribution of diffusive, long-distance scattered light due to the microroughness of the mirrors, which is not accounted for by the PSFs provided by the instrument team.
We have developed a novel analytical technique that uses eclipse images and enables us to update the existing PSFs for diffusively scattered light. No preexisting knowledge on the shape of the missing part of the PSF is required. Applying this technique to the PSF provided by the instrument team, combined with analyzing 50 partial solar eclipses, shows that an additional 5% of the light is scattered farther away than 100 arcsec.
These missing 5% result in that the intensity of bright structures, such as active regions, is increased by an additional 5% as compared to AIA images deconvolved with the original PSFs. However, the intensity of dark structures, such as coronal holes, is decreased by about 40% as compared to AIA images deconvolved with the original PSFs. Our results demonstrate that for dark structures such as coronal holes, coronal dimmings, and filament channels, taking into account and correcting for the long-distance scattered light is essential.
We study the energy distributions of nanoflares in quiet Sun regions, using Differential Emission Measure (DEM) analysis of observations from the 6 EUV filters of the Atmospheric Imaging Assembly (AIA) onboard the Solar Dynamics Observatory (SDO). In total, we analyzed 30 sets of AIA/SDO image series distributed evenly between the years 2011 and 2018 to characterize the nanoflare frequency distribution and their contribution to coronal heating throughout different levels of solar activity during solar cycle 23. Each series covers a $400''\times 400''$ field-of-view close to disc center over an observation time of two hours at the full AIA cadence of 12 seconds. DEM analysis was used to derive the emission measure and temperature evolution for each pixel. The nanoflare frequency distribution was then extracted from the DEM results for each data set by a threshold-based algorithm developed for the AIA data characteristics.
We find that the combined nanoflare frequencies follow a power-law distribution with a power-law index $\alpha = 2.3$ that covers five orders of magnitude in event energies ($10^{23}$ to $10^{28}$ erg). The power-law index obtained from individual data sets shows only minimal variation over the multi-year period and no significant correlation to solar activity. The steep slope ($\alpha>2$) suggests that the dominant energy contribution resides in the small flare events (nanoflares). However, we find that the combined energy flux from all the detected events is at least an order of magnitude too small to account for the heating requirement of the solar corona.
Understanding the energy dissipation in plasmas with low collisionality such as the solar wind is still a matter of ongoing research. While magnetic reconnection and turbulence are processes that can produce the appropriate conditions for heating and energy dissipation at subptroton scales, the energy distribution during 3D reconnection events that occur from a turbulent cascade is not entirely clear. To shed some light on this topic, we use an explicit fully kinetic particle-in-cell code to simulate 3D small scale magnetic reconnection events forming in anisotropic and Alfvénic decaying turbulence. We define a set of indicators to find reconnection sites in our simulation based on intensity thresholds. According to the application of these indicators, we identify the occurrence of reconnection events in the simulation domain and analyse one of these events in detail. The event involves two reconnecting flux ropes, and it is highly dynamic and asymmetric. We study the profiles of plasma and magnetic-field fluctuations recorded along artificial-spacecraft trajectories passing near and through the reconnection region as well as the energy exchange between particles and fields during this event. Our results suggest that the distribution of the internal energy is controlled by the region between the reconnecting flux ropes whereas the kinetic energy is associated to the inner part of the flux ropes.
Fast-drift solar radio bursts' exciter velocities have been well studied by analysing type III and type J bursts. These bursts are produced by electron beams travel along open and closed coronal flux tubes. It is thought that electron beams travelling along different magnetic field structures have similar acceleration properties although it has not systematically been tested using radio bursts. By analysing a solar radio noise storm observed by the Low-frequency-array (LOFAR) on the 10th of April 2019, we identified 27 type-III and 27 type-J busts during a solar radio bursts and derived exciter velocities for all identified radio bursts from their frequency draft rates. The comparison shows their speeds are similar, inferring that electron beams experience a similar acceleration process in closed and open flux tubes during the same solar activity event.
We derived the ambient plasma density models that varied along the ascending leg of coronal loops and solar altitude by analysing selected 17 type J bursts. By estimating the density scale height, we inferred physical parameters of large coronal magnetic loops roughly 0.7 to 1.5 solar radii above the photosphere. Coronal loop tops had temperatures around 1.3 MK, pressures around 2.1 dynes/cm^2 and minimum magnetic field strength around 0.22 G. The physical parameters of such large loops are historically ill-defined.
We investigate the generation of mass flux due to a torsional Alfvén pulse, as observed in e.g. photospheric magnetic bright points (MBPs). A flux tube model is developed, with the waves introduced at the lower, photospheric boundary of the tube as a magnetic shear perturbation. Due to the nature of MBPs we simplify the model by using the zero-beta approximation for the plasma inside the tube. We derive that the presence of torsional Alfvén waves can result in field-aligned plasma flux formed non-linearly due to the Lorentz force generated by the perturbations. Thus the model is consistent with jet formation observed in the lower solar atmosphere. The formation of the rising mass flux may even be a viable contribution to the generation of chromospheric mass transport, playing potential roles in the form of localised lower solar atmospheric jets. The analytical results are demonstrated by an example of the type of Alfvén wave perturbation that one might expect to observe, and comparison is made with properties of spicules known from observations.
The latest expansions to the standard flare model in three dimensions (Aulanier & Dudík, 2019) led to identification of geometries in which field lines reconnect during eruptive flares. One of these geometries is the magnetic ‘ar-rf’ reconnection between the erupting flux rope and surrounding field lines. It occurs at ribbon hooks and leads to drift of flux rope footpoints across the solar surface. We report on observations of signatures of this reconnection geometry in multiple eruptive flares observed by the Atmospheric Imaging Assembly onboard SDO. Apart from drifting of CME footpoints, its presence is manifested e.g., in the conversion of filament strands to flare loops, spatial expansion of a core dimming region, and formation of newly-discovered saddle-shaped arcades of flare loops. We demonstrate how can the evolution and morphology of flare ribbons indicate the nature of processes powering flares and evolution of CMEs.
Observations have revealed the diffusive nature of solar coronal plasma in the form of solar flares, coronal mass ejections, jets--manifestation of magnetic reconnections (MRs). The onset of reconnection in a perfectly conducting plasma like the solar corona requires the generation of small scales in consequence of large scale dynamics, eventually leading to a locally reduced characteristic length scale of the magnetic field variability. At such small scales, the standard magnetohydrodynamics is not valid and the Hall-magnetohydrodynamics (Hall MHD) takes over. Hall MHD gives the faster reconnection as well as resolves the details of dynamics at small scales. To explore the reconnection in Hall MHD, we have successfully extended the computational model EULAG-MHD to include the Hall forcing and reported the evolution of three-dimensional (3D) coherent magnetic structures recently. Simulations of evolution of a magnetic flux rope from solar corona like sheared magnetic arcades in the presence and absence of the Hall forcing have revealed that the rope evolves through intermediate complex structures, ultimately breaking locally because of reconnections in the presence of Hall forcing. Interestingly, the breakage occurs earlier in the presence of the Hall term, signifying faster dynamics leading to magnetic topologies favorable for reconnections.
The propagation of magnetoacoustic waves about a 2D magnetic X-point has revealed the existence of oscillatory reconnection, which is a series of horizontal and vertical current sheets with associated changes in magnetic connectivity. Oscillatory reconnection has been proposed as a wave-generation mechanism to explain some of high-speed, quasi-periodic outflows/jets in the solar atmosphere, as well as one possible physical mechanism behind quasi-periodic pulsations (QPPs). In this study we expand the results of McLaughlin et al. (2009) by performing a parameter study over a wide range of base temperatures. We solve the full set of 2D MHD equations for a magnetic X-point with the use of the PLUTO code, with explicit resistivity included. Through a nonlinear wave, we initiate the collapse of the X-point into a current sheet, initiating oscillatory reconnection for systems of different base temperatures. We study the evolution of plasma beta and its effects on the oscillatory process. By increasing the base temperature of the system, we see that both the amplitude and the period of the oscillating current density profile change. Finally, we will discuss how thermal conduction affects the temperature evolution of our systems, and by extension the final non-potential state of our systems.
Magnetic helicity is a physical quantity of great importance in the study of magnetized plasmas as it is conserved in ideal magneto-hydrodynamics and slowly deteriorating in non-ideal conditions such as magnetic reconnection. A meaningful way of defining a density for magnetic helicity is through field line helicity, which, in solar conditions, is expressed by relative field line helicity (RFLH). In this work we study in detail the behaviour of RFLH in a solar active region (AR) for the first time. The target AR is the large, well-studied, eruptive AR 11158. The computation of RFLH is based on a high-quality non-linear force-free reconstruction of the AR coronal magnetic field, and on the recent developments in its computational methodology. The derived photospheric morphology of RFLH is very different than that of the magnetic field or the electrical current. The large decrease in the value of helicity during an X-class flare of the AR is also depicted in the photospheric morphology of RFLH. Moreover, the area of the RFLH decrease coincides with the location of a flux rope, that is, of the magnetic structure that later erupted. The use of RFLH can thus provide important information about the value and location of the magnetic helicity expelled from the solar atmosphere during eruptive events.
Twist is routinely used to quantify the location of flux ropes and to understand their evolution. At the Sun, we rely on the quantity Tw that describes how much two infinitesimally close field lines wind about each other due to its simple derivation from parallel current. In this work we present a simple method for the identification of a flux rope axis and the calculation of the winding number for its field lines. The behaviour of this metric is explored in comparison to Tw.
Chromospheric oscillations with durations of approximately 3 minutes are prominent and thought to be related to the acoustic cut-off frequency of the medium. Here we used data from the CRISP instrument at the Swedish Solar Telescope and the Solar Dynamics Observatory to investigate intensity oscillations in an active region around the time of an M-class flare. Power spectrum fitting was used to characterise the locations and typical periods of the oscillations. Comparing results from before and after the impulsive phase of the flare, both the locations of the oscillatory signals and their typical periods were seen to change, with some periods seen to increase from ~100s to ~200s. The cut-off frequency can be linked to the magnetic field inclination, meaning these results could reveal how the flare has changed the magnetic environment in this active region.
Polarization properties of solar radio emissions are known to be a rich source of information about the solar emission mechanisms and the magnetic field topology. Nonetheless, largely due to technical challenges, polarimetric imaging observations of the Sun at low radio frequencies have remained very rare. The degree of polarization of the solar radio emission varies dramatically over time, frequency and also in spatial structure depending on emission mechanism. The radio bursts show moderate to high degree of circular polarization and the quiet sun thermal emissions show very low degree of circular polarization (~<1%). When it becomes possible, detection of very low circular polarisation from quiet Sun thermal emission will be an important tool to measure quiet Sun coronal magnetic field. Simultaneous measurement of linear and circular polarisation from active emissions are important to understand the quasi-longitudinal and quasi-transverse propagation and will direct probe the magnetic field geometry. Due to large Faraday rotation, narrow bandwidth observations are allowing us to detect possibly the first ever linearly polarised emission from radio bursts at low-frequencies. Perhaps the most rewarding, and also challenging, will be the polarimetric observations of gyrosynchrotron emission from CME plasma, which will allow us to model the CME plasma parameters unambiguously. We are developing a radio interferometric imaging pipeline for snapshot spectroscopic polarimeteric solar images to enable such studies. Here we summarise its current status and showcase some early results. While this pipeline is optimised for the Murchison Widefield array, a SKA-low precursor, it can be adapted for the SKA-Low.
STIX on board Solar Orbiter uses an indirect imaging system to measure flare location, size and morphology. Pairs of tungsten grids create Moiré fringes on its coarsely pixelated CdTe detectors. Images are then reconstructed on the ground, using sophisticated imaging algorithms, after the full pixel has been download. STIX therefore uses a dedicated sub-collimator to estimate a rough (within a few arcminutes), but unambiguous, flare location on board in near real time. The Coarse Flare Locator (CFL) consists of a single grid with a specific pattern which selectively illuminates pixels of a dedicated detector based on the source location. The correlation between the counts in the pixels of this detector and a look up table of pre-caculated expectations allows the location to be estimated promptly, within the constraints of on board processing. Using the downloaded measured counts in each pixel the coarse flare location can also be reconstructed on the ground. This allows for more sophisticated algorithms which require greater computational power than is available on board; greater flexibility as to which time and energy intervals are combined; and more careful background subtraction. The first estimates of STIX flare locations calculated using the STIX Ground Processing Software (GSW) from data taken during the first year of STIX operations are presented here. Comparisons are made to the expected active region and source locations, using data from several other instruments. Pending a successful flight software update the on board location estimates will also be analysed and compared with expectations.
The X1.6 flare observed on 22 October 2014 (SOL2014-10-22T14:28) was among the strongest flares occurred in the great and magnetically complex active region NOAA 12192. It was a confined flare, without an accompanying CME, despite the large amount of released energy.
We attempt to deepen our understanding of the magnetic field configuration of NOAA 12192. We analyzed the polarization signatures during the flare using spectro-polarimetric data acquired by the IBIS/DST instrument along the photospheric Fe I 617.3 nm and the chromospheric Ca II 854.2 nm lines in a time interval immediately following the peak of the X1.6 flare. The results obtained provided evidence of significant changes in the magnetic field configuration during the analyzed time interval.
We report the first unambiguous observational evidence in the radio range of
the reflection of a coronal shock wave at the boundary of an equatorial coronal hole.
The eruption occurred on 2011 August 11 above active region NOAA 11263 and
was accompanied by an EUV wave, as evinced by AIA/SDO and EUVI/STEREO
observations, and an anomalous reverse-drifting metric type II radio burst,
interpreted as a signature of the reflected shock. By combining EUV images
from AIA and EUVI with radio observations obtained by the Nancay Radioheliograph (NRH),
we show that the reverse-drifting type II radio emission was produced at the
intersection of the shock front, reflected at a coronal hole boundary, with an
intervening low-Alfvén speed region characterised by an open field configuration.
Moreover, we provide a data-driven reconstruction of the
spatio-temporal evolution of the shock-accelerated electron beams produced
by the reflected shock.
Solar eruptions, such as flares and coronal mass ejections (CME), are key drivers of space weather phenomena. CMEs are large plasma eruptions, with magnetic flux ropes frozen-in the plasma. They can travel within the heliosphere with speeds from a few hundred up to 1000 km/s and can have a profound impact on the near-Earth environment, as well as human activity in space and on ground. Modelling and successfully reconstructing CMEs is essential for space weather forecasting purposes. In this study we investigate the implementation of the spheromak CME-type flux rope model used in EUHFORIA (EUropean Heliospheric FORecasting Information Asset). To this purpose we select a CME event from the 6th of January 2013 as a test case. We translate the observable properties of the CME into model inputs. Particular attention is given in translating the observed angular widths of the CME, as captured in white-light images, to a spheromak radius. In addition, we investigate the insertion angle of the spheromak necessary to capture the observed magnetic field topology at the source region. To assess the model output, we compare it with in-situ observations at two spacecraft locations, Venus Express (~0.7 AU) and STEREO-A (1 AU), which were radially aligned during the eruption. To further understand the modelling results we conducted detailed investigations on the dynamics of the magnetic structure as it propagates.
Turbulence in space and astrophysical plasmas is an intrinsic multiscale phenomenon, which involves nonlinear coupling across different temporal and spatial scales. As a result, the physical mechanisms responsible for the turbulent dissipation and the heating of the plasma below the proton characteristic scales remain largely unknown. In this talk, we will present recent results from a statistical multiscale study of Hall-MHD and hybrid-kinetic numerical simulations of plasma turbulence, performed employing Iterative Filtering, a technique designed for the analysis of nonstationary nonlinear multidimensional signals. A spatial decomposition reveals that turbulence at sub-proton scales is highly intermittent, formed by localized magnetic structures and/or perturbations organized in a filamented network where dissipation is enhanced. Further spatiotemporal analysis shows that such perturbations (with temporal frequencies smaller or comparable to the ion-cyclotron frequency) cannot be described in terms of either kinetic Alfvén or ion-cyclotron waves. Implications of these results and comparison with solar wind turbulence observations will be discussed.
The sheath regions driven by coronal mass ejections (CMEs) are large-scale heliospheric structures. Turbulent and compressed sheaths could contribute to the acceleration of charged particles in interplanetary space, but their internal structure and its relation to energization process is still poorly understood. We report here the analysis based on observations by Solar Orbiter, BepiColombo and the L1 spacecraft to explore the structure of a coronal mass ejection (CME)-driven sheath and enhancements of energetic ions that occurred on April 19-20, 2020. Our detailed analysis of the magnetic field, plasma and particle observations show that the enhancements were related to the Heliospheric Current Sheet crossings related to the reconnecting currents sheets in the vicinity of the shock and a mini flux rope that was compressed at the leading edge of the CME ejecta. This study highlights the importance of smaller-scale sheath structures for the energization process. These structures likely formed already closer to the Sun and were swept and compressed from the upstream wind past the shock into the sheath. The upcoming observations by the recent missions (Solar Orbiter, Parker Solar Probe and BepiColombo) provide an excellent opportunity to explore further their role.
Coronal holes (CHs) are regions with open magnetic field topology in the solar corona. They are characterized by lower densities and temperatures compared to the ambient solar environment. Further, they are the source regions of high speed solar wind streams (HSSs), which propagate through the interplanetary space. Throughout the years, many authors have performed statistical studies comparing the CH properties and the characteristics of the HSSs at Earth in order to understand their relationship. This topic is of utmost importance for modelling the solar wind environment in interplanetary space as well as for space weather predictions.
In this study, we perform a statistical analysis of a set of 45 CHs during a period of solar minimum activity. We focus on the geometrical shape of the CHs and we divide our sample in different groups based on various geometrical criteria. We then examine the relationship of each group with the HSS peak velocity at Earth. Our results show that the HSS peak velocity in situ is better constrained by CHs of specific properties. We further quantify the geometrical complexity of the CHs by employing two different ways: (a) by defining a ratio of geometrical properties and (b) by calculating their fractal dimension.
Sunspot areas are important quantities that can be obtained from the analysis of the images of the solar photosphere. In particular, sunspot areas extracted from historical solar drawings are very useful due to its strong correlation with other solar activity indices as the Group Number or the Sunspot Number (related to the solar irradiance too). Usually, sunspot areas corrected from foreshortening (in millionths of solar hemisphere, or msh) are determined using the well-known equation
$A_{M}= \frac{10^{6} A_{S}}{2\pi R^{2} \cos\rho}$
where $A_{S}$ is the sunspot area measured directly on the image, $R$, the radius of the solar disk and $\rho$ the angle between the direction of the centre of the solar disk and the direction of the sunspot.
We have analysed the uncertainties in the measurement of $A_{M}$ due to the different factors included in above equation, with special interest in the influence of the binarization threshold in the measure of $A_{S}$. Moreover, as the equation is an approximation valid for relatively small sunspots where the angle $\rho$ is the same for all the sunspot surface, we have analysed its validity for unrestricted size sunspots of circular and elliptical shapes.
Coronal mass ejections (CMEs) and stream interaction regions (SIRs) are different large-scale structures in the solar wind. When interacting with Earth, they may cause the most severe Space Weather effects. Between solar wind and Earth’s magnetosphere also other possible geoeffective phenomena are generated, namely “magnetosheath jets”. They are defined mainly as dynamic pressure enhancements and constitute a significant coupling effect between the solar wind and the magnetosphere of the Earth. How they are related to CMEs and SIRs is so far not explored. To shed light on this relation and on the generation of these jets in general, we present the first-ever statistical results of the jet production during CMEs and SIR times by using THEMIS data. We find that the number and total time of observed jets decrease while CMEs hit the Earth's magnetic field. On the other hand, the number of jets increases during SIR phases. We discuss possible physical processes to explain these statistical differences.
This paper presents the results of the analysis of the dynamics of coronal holes on the Sun during the period May 13, 2010- May 13, 2021. In our study used images in the extreme ultraviolet in the Fe XII, XXIV line (193 Å) obtained with the Atmospheric Imager Assembly of the Solar Dynamics Observatory (AIA/SDO). To localize coronal holes and determine their areas, we used the Heliophysics Event Knowledgebase (HEK), which is available at http://www.lmsal.com/hek/hek_isolsearch.html . Information on coronal holes was extracted with the Spatial Possibilistic Clustering Algorithm (SPoCA). The separation of all coronal holes of the considered period into polar and non-polar ones showed that the daily total area of polar coronal holes increases at the minima of solar activity and decreases at the maximum of the cycle. This is consistent with the general concept of polar coronal holes as the main source of the solar dipole magnetic field. There is an asymmetry in the areas of polar coronal holes in the northern and southern hemispheres. It is shown that the areas of nonpolar coronal holes vary quasi-synchronous with the sunspot activity of the Sun, which suggests the existence of a physical connection between these two phenomena. Apparently, the nature of the magnetic fields of polar and non-polar coronal holes is different. Non-polar coronal holes are possibly very high loops that close through the corona in other regions of the Sun, while polar coronal holes extend far into the heliosphere.
The polar precursor method is widely considered to be the most robust physically motivated method to predict the strengths of an upcoming solar cycle. It uses in form of indicators, the magnetic field concentrated near the poles around sunspot minimum. Here, we present an extensive performance analysis of various such predictors, based on observational data like (WSO magnetograms, MWO polar faculae counts and Pulkovo A(t) index) and outputs (global dipole moment) of various existing flux transport dynamo models. We have calculated Pearson correlation coefficients (r) of the predictors with the next cycle amplitude as a function of time measured from solar cycle maximum and polar field reversal. Setting r = 0.8 as a lower limit for acceptable predictions, we find that observations and models alike indicate that the earliest time when the polar predictor can be safely used is 4 years after polar field reversal. This is typically 2 to 3 years before the solar minimum and about 7 years before the predicted maximum. Re-evaluating the predictors another 3 years later, at the time of solar minimum, further increases the correlation level to r > 0.9. As an illustration of the result, we determine the predicted amplitude of Cycle 25 based on the value of the WSO polar field at the official minimum date of December 2019 as 126 ± 3. A forecast based on the value in early 2017, 4 years after polar reversal would have only differed from this final prediction by ~ 3.1 %.
We performed a digitization of maximum magnetic field measurements in sunspots. The original data were acquired as drawings at the Crimean Astrophysical Observatory of the Russian Academy of Sciences (CrAO RAS). About 1000 sunspots observed in 2014 were analyzed. The data were compared to the corresponding measurements from the SDO/HMI instrument. For the same sunspot, the maximum modulus of the magnetic field derived at CrAO was compared to the corresponding value from HMI. The Crimean data and the space-based data were found to be in direct proportion to each other. A linear approximation over the entire range of measurements (1–4) kilogauss (kG) shows a Pearson correlation coefficient of 0.71 (with the 95 % confidence boundaries of 0.68–0.74) and a slope of linear regression of 0.65±0.02. A linear approximation over the range of strong fields B(CrAO) > 1.8 kG gives a similar correlation, however the slope of linear regression is far closer to unity and constitutes 0.90. In the range of weak fields B(CrAO) < 1.8 kG, a non-linear deviation (exceeding) of the space-based data is observed. Non-linearity can be explained, in part, by a specific routine of the magnetic field measurements at CrAO, however further investigations are needed to explore sources of possible non-linearity in the HMI data. The Crimean measurements of the maximum magnetic field in sunspots are concluded to be in good agreement with the corresponding SDO/HMI measurements, and therefore they can be used for scientific purposes.
One of the methods to predict the future solar activity is the minimum - maximum method, which is based on a linear relationship between relative sunspot number in the minimum and maximum epochs of solar cycles. It belongs to the precursor class of the solar activity forecasting methods. In present work we apply a modified version of this method using data not only from the minimum year, but also from a couple of years before and after the minimum. The new version of the 13-month smoothed monthly total sunspot number data set from SILSO-SIDC is used. We investigate the value of the correlation coefficient of the mentioned relationship as a function of the time lag around the solar minimum. Further, a statistical significance of the results and inclusion/exclusion of the curious solar cycle no. 19 are discussed. For the next solar maximum of the cycle no. 25 we predict a similar amplitude as the previous one, or even something lower. This is in accordance with the overall middle-term lowering of the solar activity after the secular maximum in the 20th century and consistent with the Gleissberg period of the solar activity. The reliability of the method is experimentally checked by applying it to reconstruct a couple of previous solar cycle maxima, using the earlier data. Finally, the minimum-maximum method and its results are discussed in the context of the well-known empirical findings: the extended solar cycle and the Waldmeier effect, as well as various solar dynamo models.
The 11-Year solar cycle is driven by the sun’s magnetic field. The sunspot number is the most-common long term index of solar activity and prediction of its amplitude can help to understand the effects of space weather & solar activity. Previous studies have shown that analyzing the solar activity of the two hemispheres separately instead of the full sun can provide more detailed information on the activity evolution. However, the existing Hemispheric Sunspot Number(HSN) series (1945 onwards) is too short for the purpose of solar cycle predictions. Based on a newly created HSN catalogue for the time range 1874-2020 (Veronig et al. 2021) that is compatible with the International Sunspot Number from WDC-SILSO, we investigate the evolution of the solar cycle for the two hemispheres, and demonstrate that empirical solar cycle prediction methods can be enhanced by investigating the solar cycle dynamics in terms of HSN. We develop a method for predicting the solar cycle amplitude based on the peak growth rate in the ascending phase of the cycle using HSN for cycles 12-24. We show that using this technique, the sum of the predictions (North + South) of the two hemisphere give better estimates of the cycle amplitude than the Total Sunspot Numbers. In addition, we estimate the cycle peaks with 1st order and 3rd order regressions and find that the HSN provide better estimates of cycle peak than total sunspot numbers with the obtained correlations lying in the range r = 0.8-0.9 depending on the applied smoothing window
The quasi-biennial oscillation (QBO) is a low amplitude oscillatory signal commonly seen in solar activity proxies and may hold the key to a greater understanding of the solar dynamo. This will help us mitigate the risks that come with space weather which is driven by the solar magnetic field. In addition, mid-cycle oscillations have been observed on other stars, making the impact of this work extend beyond our own solar system. We use helioseismology to probe the solar interior by examining frequency shifts of p-modes to isolate the QBO and its associated periodicity. We also investigate the p-modes’ spatial and frequency distribution, and examine how these distributions change over Cycles 23 and 24. We use data from the Global Oscillations Network Group, Michelson Doppler Imager and Helioseismic & Magnetic Imager in the intermediate-degree range, as well as solar activity proxies to investigate Cycles 21-24. We use Empirical Mode Decomposition which is adept at picking out quasi-oscillatory signals where the signal is allowed to vary in period, shape, phase, and amplitude. We find evidence of the QBO in both Cycles 23 and 24, although it is less significant in Cycle 24, which raises the possibility of a multiplicative relationship between the activity of a solar cycle and the presence of the QBO. We also see the evidence of the QBO across depths from 0.2-0.95 solar radii, suggesting that the magnetic field driving the QBO is likely to be located in the near surface region.
To find out observational evidences for the turbulent component of the solar dynamo in the convective zone is a very challenging problem because the dynamo action is hidden below the photosphere. Here we present results of a statistical study of active regions (ARs) with strong flares (>X1.0) occurred during the 23rd and 24th solar cycles. A suggested magneto-morphological classification of ARs allowed us to diagnose the degree of intervention of the turbulent (mid-scale and small-scale) component of the dynamo. We found that in 72% of cases, the strong-flaring ARs do not comply empirical laws of the global dynamo (the Hale polarity law, the Joy's law, the leading spot prevalence rule; ARs-"violators") and therefore they may be attributed to the influence of the turbulent dynamo action inside the convective zone on scales of typical ARs. We found that strongest flares occur in the ARs-"violators", so the flaring capability of the Sun is controlled by the turbulent component of dynamo. ARs-"violators" with strongest flares tend to happen during the second maximum and the descending phase, when the toroidal field ceases and the turbulent component of the dynamo should be more pronounced. These observational results are in consensus with a concept of essential role of non-linearity and turbulent intermittency in the magnetic fields generation inside the convective zone, which follows from simulations of dynamo.
Why the atmosphere of the Sun is orders of magnitudes hotter than its surface is a long standing question in Solar Physics. Over the years, many studies have looked at the potential role of MHD waves in sustaining these high temperatures. In this study, we use 3D MHD simulations to investigate (driven) Alfvenic waves in a coronal loop. Due to the radial density profile, resonant absorption (or mode coupling) and phase mixing take part in the boundaries of the flux tube and the large velocity shears are subject to the Kelvin Helmholtz instability (KHI). The combination of these effects leads to enhanced energy dissipation and wave heating. By considering a variety of wave drivers and coronal loop profiles, we determine when this energy release is sufficient to balance radiative losses.
Recent observational and theoretical studies indicate that the damping of solar coronal loop oscillations depends on the oscillation amplitude. We consider the mechanisms of linear resonant absorption and of nonlinear damping due to the development of the Kelvin-Helmholtz instability. We confront theoretical predictions from these models with observed data in the plane of observables defined by the damping ratio and the oscillation amplitude. The structure of the Bayesian evidence in this plane displays a clear separation between the regions where each model is more plausible relative to the other. There is qualitative agreement between the regions of highest marginal likelihood and Bayes factor for the nonlinear damping model and the arrangement of observed data. A quantitative application to 101 loop oscillation cases observed with SDO/AIA results in the marginal likelihood for nonlinear damping being larger in the majority of them. The cases with conclusive evidence for nonlinear damping outnumber considerably those in favor of linear resonant absorption.
High-resolution solar observations from both space-borne and ground-based telescopes have revealed ubiquitous photospheric vortical motions in quiet, as well as in active regions. In observations of the chromosphere, obtained in spectral lines, such as the Hα and the Ca II IR, they appear as spiral-shaped or circular dark patches. These so called “chromospheric swirls” are considered to be of great significance due to their ubiquity, and to their suggested contribution to the energy transfer from the sub-photospheric layers to the transition region and corona. Therefore, statistical information concerning their population and a number of significant physical properties, such as radii, lifetimes and line-of-sight velocities are imperative in order to understand their nature and estimate the amount of the upwards energy transfer. We have developed a novel, automated chromospheric swirl detection method based on their morphological characteristics, in an attempt to complement visual inspection methods and velocity field derivation techniques used to date, with a more reliable to chromospheric observations method. We will be presenting the designed algorithm, and its evaluation on different observational datasets in several chromospheric spectral lines, obtained with the CRisp Imaging SpectroPolarimeter (CRISP) and the CHROMosheric Imaging Spectrometer (CHROMIS) of the Swedish 1-m Solar Telescope (SST). In addition to the swirl detection results, various parameters derived from a multi-line and multi-wavelength analysis conducted on detected swirls, within selected areas, will be presented and discussed.
ALMA millimeter wavelength images of the Sun show significant correspondence with the solar magnetograms. We analyze the observed correspondence by comparing ALMA solar images taken at 1.2 and 3.0 mm with SDO/HMI line-of-sight magnetograms. We find that the active regions and the chromospheric network show a positive correlation where the brightness temperature increases with the line-of-sight magnetic field strength, while sunspots display the opposite behavior with a negative correlation. On the other hand, quiet Sun regions do not show any dependence of brightness temperature with the magnetic field. Several radiation mechanisms are explored to explain the observed (anti)correlations. Thermal free-free emission is given as the most probable explanation and the main contributor to the observed correlations with enhanced heating in the active regions and a decrease of temperature in the sunspots due to the suppression of convection by the magnetic field.
We revisit the so-called levitation-condensation mechanism for the \textit{ab-inito} formation of solar prominences: cool and dense clouds in the million-degree solar atmosphere. A flux rope is formed in response to the deformation of a force-free coronal arcade by controlled magnetic footpoint motions and subsequent reconnection. Existing coronal plasma gets lifted within the forming rope, therein isolating a collection of matter now more dense than its immediate surroundings. This denser region ultimately suffers a thermal instability driven by radiative losses and a prominence forms. Our modern open-source grid-adaptive simulation code [amrvac.org] enables a resolution of 5.6 km within a 24 Mm x 25 Mm domain size; the full global flux rope dynamics and local plasma dynamics are captured in unprecedented detail. Our 2.5D simulation demonstrates that the thermal runaway condensation can happen at any location, not solely in the bottom part of the flux rope where the majority of prominence material is assumed to reside. Intricate thermodynamic evolution and shearing flows develop spontaneously, themselves inducing further fine-scale (magneto)hydrodynamic instabilities. Our analysis touches base with advanced linear magnetohydrodynamic stability theory, e.g. with the Convective Continuum Instability or CCI process as well as with in-situ thermal instability studies. We find that condensing prominence plasma evolves according to the internal pressure and density gradients as found previously for coronal rain condensations, but also misalignments therein suggesting the relevance of the Rayleigh-Taylor instability or RTI process in 3D. We also find evidence for resistively-driven dynamics in the prominence body, in close analogy with analytical predictions.
The solar atmosphere is hotter than predicted by assuming radiative equilibrium. This is most obviously evidenced by the high temperature of the solar corona, but the bulk of the energy deposition happens already down in the much cooler chromosphere. While in recent years we have gain detailed understanding of many important processes that must be at work in the chromosphere, also from numerical simulations, their exact contribution to the total energy budget remains unclear.
Chromospheric heating or cooling can be estimated by calculating the radiative losses whenever a model atmosphere is available. Most comparisons between simulations and observations have used canonical values of radiative losses that have been derived from 1D models of spato-temporal averages of solar spectra (e.g., FAL / VAL models). Such approach cannot capture the high complexity and fine structures that is observed in high resolution observations. Recent studies have evidenced that spatially resolved radiative cooling can be up to five times higher in active regions than those canonical values that are usually assumed.
In this talk, we present spatially resolved radiative cooling rates computed from the inversion of high spatial resolution chromospheric datasets observed with the Swedish 1-m Solar Telescope in Ca II K, 8542 and Fe I 6301/6302. We study the distribution of radiative cooling across the FOV in different targets in active regions and in quiet-Sun. Our results will help modellers to set better constraints on theoretical predictions and models.
Network jets at transition region temperatures of ca. 0.1 MK have been observed to be widespread enough to provide substantial mass and energy to the upper solar atmosphere. Previous studies of this phenomena have mostly focused on near-limb and broadband imagery data and ascribed propagating intensity disturbances as mass motions. Thus, the nature of plasma flows in these jets and their driving mechanism remain unclear. Using co-aligned IRIS and SDO/HMI data, we present observations of a small-scale jet located within a coronal hole at disc-center. The analysis of the event spectra of the Si IV line at 1394 Å showed clear blue-shifts at transition region temperatures along the upper portion of the jet. The jet can be traced to its base where heightened chromospheric activity in Mg II overlaps areas of strong line-of-sight magnetic field concentrations. While single-gaussian fits only show obvious blue-shifts near the top of the jet, closer inspection of the individual spectra reveals a double-peaked profile along the spire of the jet. Near the base of the jet, a weak, blue-shifted secondary component exists. This secondary component, exhibiting flow speeds of 30-60 km/s, becomes stronger farther along the jet from its base, eventually influencing the single-gaussian fits to show blue-shifts of the Si IV spectral line profiles. This observation allows for a unique investigation of the true mass motions of a jet clearly identified in the transition region and down into the chromosphere, where it can be connected to changes in the underlying magnetic field.
Localized brightenings observed in extreme-ultraviolet (EUV) images, are generally interpreted as signatures of micro-or nanoflares occurring in the transition region or lower corona. These brightenings are omnipresent and hence, could well play a major role in heating up the solar corona. Recent observations with the Extreme Ultraviolet Imager (EUI) on board Solar Orbiter have revealed such localized brightenings (‘campfires’) down to an unprecedented size of only of 0.08 Mm^2 (2 EUI pixels). These are the smallest such events yet observed in the quiet-Sun corona. In our study, we find a number of these loop-like brightenings to host propagating features that are manifestations of the internal dynamics. Typically, the propagation speeds range from 30 km/s to 60 km/s. Assuming the loop plasma to be at million Kelvin, these apparent motions would be below the local sound speed, but still quite substantial. Most interestingly, we find non-trivial propagation characteristics, in particular bifurcation, merging, and reflection. These signatures could provide important insights about the dynamic response of the (loop) plasma to the heating events and the location of the heating events themselves. For example, initiation of the brightening on one side of the loop and reflection at the other suggests energization at the footpoint, while an origin of the propagating feature near the apex would be consistent with heating near the top of the bundle of magnetic fieldlines defining the loop. We will discuss these observational results and put them into the context of recent 3D modeling of the small transient brightenings.
Small scale solar vortices are ubiquitous in the photosphere, and they are believed to organize the magnetic fluxes, creating efficient conduits for energy transport and wave propagation. Another process linked to vortical flows is the generation of twisted magnetic flux tubes. In this work, the twisted magnetic flux is defined as a new typology of a solar vortex, and we applied forefront methodologies to detect both the kinetic and magnetic vortices tubes in realistic magnetoconvection simulations. Our results show that those types of vortices are found in distinct parts of the intergranular downflow. The magnetic vortices appear mostly in shear flow areas where plasma-$\beta>1$, whereas the kinetic vortices are found in low plasma-$\beta$ regions. The solar vortices present similar dynamics at different solar atmosphere levels, concentrating and perturbing the magnetic field lines. The kinetic vortices show upward jets and tend to encompass high magnetic fluxes; thereby, their dynamics is mainly dominated by magnetic forces. Based on the magnetic and kinetic energy ratio obtained for magnetic vortices, we determined that they can be classified into two distinct types, with considerable differences in the overall geometry of the magnetic field line. Our results indicate that the presence of rotational motion in the flow is not necessary for the appearance of magnetic vortices.
Five years ago, regular observations of the Sun with the Atacama Large Millimeter/sub-millimeter Array (ALMA) started. Since then, an increasing number of data sets have been acquired. At the same time, the Solar ALMA Pipeline (SoAP) for processing these data sets has been improved substantially. As a result, the first version of the Solar ALMA Science Archive (SALSA) was constructed. The aim of SALSA, being the final product of the now concluding ERC-funded Solar ALMA project, is to provide science-ready ALMA data to solar physicists. The contained data is mostly comprised of high-cadence (1-2s) time series of millimetre continuum images for different receiver bands and solar targets. A particular advantage is that these ALMA maps provide direct measurements of (brightness) temperatures in different chromospheric layers that are complementary to other chromospheric diagnostics.
After a brief introduction to the opportunities and challenges connected to observing the Sun with ALMA, examples of SALSA data and first scientific results regarding, e.g., the imprint of magnetic fields, propagating shock waves, and oscillations are presented. Finally, the diagnostic potential for the Sun and other stars and the future development of ALMA’s solar capabilities are discussed.
SDO/AIA images the full solar disk in several EUV bands that are each sensitive to coronal plasma emissions of one or more specific temperatures. We observe that when isolated active regions (ARs) are on the disk, full-disk images in some of the coronal EUV channels show the outskirts of the AR as a dark moat surrounding the AR. We will present several specific examples, selected from time periods when there was only a single AR present on the disk. Visually, moats are observed to be most prominent in the AIA 171 Angstrom band, which has the most sensitivity to emission from plasma at log10 T = 5.8. By using the emission measure distribution with temperature, we find the intensity of the moat to be most depressed over the temperature range log10 T ~ 5.7 - 6.2 for all the cases. We argue that the dark moat exists because the pressure from the strong magnetic field that splays out from the AR presses down on underlying magnetic loops, flattening those loops -- along with the lowest of the AR's own loops over the moat -- to a low altitude. Those loops, which would normally emit the bulk of the 171 Angstrom emission, are restricted to heights above the surface that are too low to have 171 Angstrom emitting plasmas sustained in them, while hotter EUV-emitting plasmas are sustained in the overlying higher-altitude long AR-rooted coronal loops. This potentially explains the low-coronal-temperature dark moats surrounding the ARs.
The plasma in the solar corona originates from the photosphere and would, therefore, be expected to have similar elemental composition. However, elements with a low first ionisation potential (FIP) have been observed to have an increased abundance in certain regions of the corona. This phenomenon is known as the FIP effect and the degree of enhancement is measured using the FIP bias parameter. The increased elemental abundance is typically observed in active regions.
In this statistical study, we analyse how the degree of enhancement varies in active regions of different sizes, ages and level of complexity. We explore whether the average FIP bias is linked to the evolution of active regions and the photospheric magnetic field at the scale of an active region. First, by exploring whether there is a correlation between average FIP bias and the total magnetic flux and age of the active region. Second, if there is an average FIP bias dependence on magnetic flux density. Third, if the average FIP bias varies depending on whether the plasma is above the leading or following polarity of an active region.
Since the discovery of the hot solar corona, a wide variety of mechanisms have been proposed for maintaining the high temperatures. The majority of these models fall into one of two broad categories, either AC (alternating current) or DC (direct current) heating. The distinction between these two groups arises from the characteristic time scales of the photospheric motions which are the source of the required energy. AC models are associated with short time scale driving and DC models with long time scales.
Despite decades of investigation, debate continues about the relative importance of AC and DC heating in different regions of the corona. In either case, the rate of energy injection is sensitive to both the imposed velocity profile (driver) and the form of the atmospheric magnetic field. The interaction of the driver with the coronal field has important consequences for energy budgets. With this in mind, I will present the results of a series of numerical simulations of coronal heating in general settings. By modifying the characteristics of an imposed, random driver, I will compare the expected energy release rates and the atmospheric response for AC and DC driving.
Both numerical simulations and observations of the solar atmosphere are limited in how small spatial variations they can resolve. The smallest processes in simulations are limited by the numerical grid employed, but the sun is under no such constraints. Therefore, observations and simulations at the same nominal resolution are not directly comparable, since sub-resolution effects not present in the simulations may still influence the observed Stokes profiles. A natural question, then, is when inferring quantities such as velocities or magnetic fields, how much is lost by not including the sub-resolution effects in the modelling? This will affect both the selection of numerical grids for simulations (to compare with observations), and the use of inversions to infer properties from observations, which often assume 1D atmospheres at the scale of each pixel. In the present work we study the effects of spatial resolution on Stokes profiles. We make use of 3D rMHD Bifrost simulations run with spatial resolutions of 6, 12, and 23 km, all starting from the same initial state. From these we compute synthetic spectra using the RH1.5D code for photospheric and chromospheric lines, which we degrade and downsample to the pixel scale of the lowest-resolution simulation (23 km). We then compare the inferred physical quantities (in particular magnetic field and line-of-sight velocities) for varying amounts of sub-pixel resolution. We find that important differences persist despite the downsampling and degradation to a lower resolution, and quantify the variation in the inferred physical quantities caused by the imprint of sub-resolution effects.
Flare-associated hot coronal loops often display compressive plasma oscillations involving a density perturbation moving back and forth between the foot points of the loop. These oscillations, sometimes referred to as, ``sloshing oscillations", exhibit properties very similar to the standing slow waves that were discovered much earlier with the SoHO/SUMER and other spectroscopic instruments. Utilising the multi-wavelength high-resolution imaging observations from SDO/AIA, we have recently shown that the sloshing oscillations eventually transform into a standing slow wave. The oscillation properties and the associated change between the two phases with respect to the evolving physical conditions within the loop, will be discussed. By analysing multiple examples, we also present the possible initial conditions under which such an oscillation may be setup.
The Nuclear Spectroscopic Telescope Array (NuSTAR) is an astrophysical X-ray telescope capable of observing the Sun with direct imaging spectroscopy providing a unique sensitivity above 2.5 keV. We use NuSTAR to investigate highly frequent and weak flares thought to contribute to heating the Sun's atmosphere particularly in active regions. I will present several X-ray microflares from a recently emerged active region, AR12721, that were observed on 2018 September 9-10 with NuSTAR. In combination with SDO/AIA, I describe the temporal, spatial, and spectral evolution of these GOES sub-A class microflares that reach temperatures above those of the surrounding active region (>5 MK). One of the microflares presented is the faintest non-thermal microflare so far observed with NuSTAR with an equivalent GOES class of A0.1. Using SDO/HMI, I also present evidence of photospheric magnetic flux cancellation/emergence at the footpoints in 8 of the NuSTAR microflares.
Energy transport by fast, non-thermal particles from primary energy release place - located in the top of flaring loop - to the loop foot-points, plays very important role in solar flares. A fully understanding of the processes of transportation, energy deposition in the chromosphere and radiative response of chrompospheric plasma requires both: high (sub-second) cadence observations and numerical models consistent with them.
The analysis of two compact solar flares with similar GOES-class (C1.1 and C1.6), but with significance differences during impulsive phase is presented. Variations of the position and the vertical extent of the energy deposition layer (EDL) as well as variations of the flaring spectra and emission intensities recorded in the H$\alpha$ hydrogen line are studied.
The variations of the HXR fluxes and H$\alpha$ intensities were well-correlated in time during the impulsive phases of the flares, and they agreed with the variations of the calculated position and vertical extent of the EDL. Impulsive variations of the H$\alpha$ emission were caused by individual, short-time episodes of energy deposition by the electron beams on various depths in the chromospheric plasma.
The compared flares were observed in H$\alpha$ line with very high time resolution (20 spectra-images per second) using the MSDP spectrograph at Bialkow Observatory (University of Wroclaw, Poland), as well as by GOES and RHESSI satellites in X-ray domain. The numerical model was calculated assuming that the external energy is delivered to the flaring loop by non-thermal electrons.
Estimates of coronal wave energies remain uncertain as a large fraction is hidden in the non-thermal line widths of emission lines. To estimate these wave energies, previous studies have taken the root mean squared wave amplitudes to be a factor of $\sqrt{2}$ greater than the non-thermal line widths. However, other studies have used different factors. To investigate this discrepancy, we consider the relation between wave amplitudes and the non-thermal line widths within a variety of 3D magnetohydrodynamic (MHD) simulations. To generate the synthetic emission required to analyse the non-thermal line widths, the forward modelling code FoMo is used. In order to estimate wave energies, an appropriate relation between the non-thermal line widths and root mean squared wave amplitudes must be found. However, evaluating this ratio to be a singular value, or even providing a lower or upper bound on it, is not realistically possible given the sensitivity it has to various MHD models. It depends on a variety of factors, including line-of-sight angles, velocity magnitudes, wave interference and exposure time. Indeed, some of our models achieved the ratios claimed in recent articles while other more complex models deviated from these values. As the ratio between wave amplitudes and non-thermal line widths is not constant across our models, this widely used method for estimating wave energy is not robust.
The purpose of our study is to deepen our understanding of the turbulence that arises from the Rayleigh Taylor Instability and leads to the formation and evolution of prominence. Quiescent prominence formed in the solar corona are cool and dense condensates comprising of varied dynamics of physical processes and scales. It is dominated by the vertical motion of flows in the upper atmosphere where the mean magnetic field is predominantly in the horizontal direction, and the magnetic pressure holds the dense suspended prominence material. Previous studies with Hinode Solar Optical Telescope's observations revealed turbulent behavior in these prominence structures having evolving rising plumes and descending pillars. We perform numerical simulations from MPI-AMRVAC to study the 2.5D Rayleigh Taylor Instability at the prominence-corona transition region, using the ideal-magnetohydrodynamic approach. High-resolution simulations achieved spatial grid resolution of $\sim 23$ km having a cadence of $\sim 0.85$ sec for $\sim 25$ min transitioning from a multi-mode perturbation instability to the non-linear regime and finally a fully turbulent region. We use statistical methods to relate that the dynamics due to the instability in quiescent prominence indicate turbulence behavior that occurs distinctly on different prominence scales for the turbulent magnetic and velocity field fluctuations.
Alfvén waves have proven to be important in a range of physical systems due to their ability to transport non-thermal energy over long distances in a magnetised plasma. This property is of specific interest in solar physics where the extreme heating of the atmosphere of the Sun remains unexplained. In an inhomogeneous plasma like a flux tube in the solar atmosphere, they manifest as incompressible torsional perturbations. However, despite evidences in the upper atmosphere, they have not been directly observed in the photosphere. Here, we report the detection of anti-phase incompressible torsional oscillations observed in a magnetic pore in the photosphere by the Interferometric BIdimensional Spectropolarimeter (IBIS). State-of-the-art numerical simulations suggest that a kink mode is a possible excitation mechanism of these waves.
The excitation of torsional waves in photospheric magnetic structures can significantly contribute to the energy transport in the solar atmosphere and the acceleration of the solar wind, especially if such signatures will be ubiquitously detected in even smaller structures with the forthcoming next generation of solar telescopes.
An automatic algorithm has been used for detection of flares in the GOES data in the period 1986-2020. The detection process starts from soft-X solar signal, provided by the NASA-GOES Satellite Network which is devoted to the surveillance of the Earth. Since flares represent one of the main events associated with Space Weather their statistics are of particular importance in this context.
The algorithm produced a database, tested with official catalogs for validation, that increased the number of detected flares by a factor of about four compared to the official GOES catalog.
In particular, the problems connected to the soft-X background flux in pre-flare conditions, multiple flares and lower intensity flares were dealt with.
In addition to briefly presenting the algorithm, we show the results of the analysis of the distributions in the last four solar cycles.
We conducted a statistical analysis of the dimming events associated with Earth-directed coronal mass ejections (CMEs) that were observed in quasi-quadrature by the SDO and STEREO satellites. We derived the properties of the dimmings as observed above the limb by STEREO EUVI and compared them with the mass and speed of the associated CMEs. The unique satellite constellation allowed us to compare our findings with the results from Dissauer et al. (2018, 2019), who studied these events observed against the solar disk by SDO AIA. Such statistics is done for the first time and confirms the close relation between characteristic dimming and CME parameters for the off-limb viewpoint. We find that the dimming areas are typically larger for off-limb observations while the total extreme ultraviolet intensity decrease is similar (c ∼ 0.6). Parameters describing the total dimming extent, i.e., off-limb area and total brightness, strongly correlate with the CME mass (c ∼ 0.7–0.8). The derivatives of these parameters show a high correlation with the CME speed (c ∼ 0.6). In addition, we studied whether the coronal dimmings can be used to identify a predominant direction of the CMEs. Using the same set of events, we estimated the dimming growth direction and compared it with modeling results of the CMEs propagation, derived from existing GCS reconstructions and provided in catalogs. Our findings suggest that coronal dimmings have the potential to provide early estimates of the Earth-directed CMEs parameters, relevant for space weather forecasts, for satellite locations at both L1 and L5.
Since the beginning of this century it became possible to make observations of solar flares in subterahertz (sub-THz) frequency range at a few frequencies in the range of 100-400 GHz. Within these observations some of M- and X-class solar events had a spectral (sub-THz) component that grew with frequency. To understand the origin of this phenomenon, we simulated the plasma density and temperature evolution in a flare loop, caused by interaction between the injected accelerated electron beams, which travel from the reconnection site in the region of the coronal loop-top down to lower layers of the solar atmosphere. The numerical code FLARIX used for simulations allowed us to define the dynamics of the flare plasma parameters at different heights, based on the equations of radiation hydrodynamics. Using the simulation results, we inferred the thermal bremsstrahlung emission in the sub-THz and X-ray ranges. The comparison of the obtained simulation results with observational data is under discussion. This work was partly supported by the RFBR (N20-52-26006), the Ministry of Education and Science (Research Work No. 0831-2019-0006), RVO: 67985815, project LM2015067: EU-ARC.CZ, 21-16508J of the Grant Agency of the Czech Republic.
The Sun frequently accelerates near-relativistic electron beams that travel out through the solar corona and interplanetary space. Undergoing wave-particle interactions with Langmuir waves, these beams are the driver for type III radio bursts, the brightest radio bursts produced by the Sun. The formation and motion of type III fine frequency structures is a puzzle but is commonly believed to be related to plasma turbulence in the solar corona and solar wind. Combining a theoretical framework with kinetic, wave-particle simulations and high-resolution radio type III observations, we quantitatively show that the fine structures are caused by the moving intense clumps of Langmuir waves in a turbulent medium. Our results show how type III fine structure can be used to remotely analyse the intensity and spectrum of compressive density fluctuations, and can infer ambient temperatures. This new plasma diagnostic for the solar corona and solar wind is at distances from the Sun where these properties normally cannot be measured, and significantly expands the current potential of solar radio emission.
We present a comprehensive multi-wavelength analysis of a coronal mass ejection (CME) associated with a M3.2 flare and filaments eruption on 8 January 2014 from the active region NOAA 11947. Observations from the AIA 171 A images reveal the origin of pre-CME arcade $\approx$ 1 hr prior to the eruptive events. After formation, the pre-CME arcade undergo through slow rise evolution with a speed $\approx$ 3 km s$^{-1}$. Subsequently, a typical ``arcade-to-bubble" transformation is observed, providing the evidence of CME in the form of bubble at lower coronal heights. Differential emission measure analysis suggests the presence of multi-thermal plasma in the bubble structure and strong plasma heating at the core of the active region. Further, the bubble undergo through a blowout expansion with a speed of $\approx$ 420 km s$^{-1}$. The blowout expansion of CME is accompanied with gradually varying EUV and X-ray emissions from the hot core and multiple type III radio bursts, indicating the magnetic reconnection as a possible triggering mechanism for CME. During the impulsive phase, we observed compact hard X-ray sources at energies up to $\approx$ 50 keV from its source region. A temporal correlation between the blowout expansion of the CME and enhanced X-ray fluxes suggests a feedback association between kinematical evolution of CME and impulsive phase of the flare. With the impulsive phase, the activation and subsequent eruption of two successive filaments take place. From these observations, we propose that CME in association with filaments eruption is a result of successive magnetic reconnections.
The soft X-ray photometric records from the GOES/XRS instruments
now approach a half century of coverage, and constitute the most
complete space-based proxy for solar flare X-ray luminosities and
energies. Observations continue with the GOES-16 and -17 and
forthcoming satellites, which use a slightly different detector
technology. Some of the most powerful earlier events saturated the
telemetry range of their ionization-chamber detectors, making it
difficult to study the event distribution function at its most
interesting top end. Over the interval 1976--2015 a total of 11
events saturated the key 1--8 Achannel, many of which were from
NOAA region 6659 in 1991. We have devised an algorithm for best
estimates of the peak fluxes for these saturated events. Based on
this new input, and our understanding of the calibration issues for
GOES-15 and earlier, we discuss the event distribution function
(e.g. Aschwanden & Freeland, 2012) looking for evidence of a
downward break in the event distribution in the vicinity of magnitude
X10. Note that the absolute calibration of this level is under
investigation at present, but this does not concern the relative
magnitude distribution. Any departure from the power law will
crucially affect our understanding of ``superflare'' occurrence on
the Sun.
Solar flares and coronal mass ejections (CME) are the most powerful manifestations of solar activity. Both phenomena associated with the evolution of the spatial structure of the magnetic field of active regions (AR). It is known that not all powerful flares accompanied by CME. In some cases, CME are observed, associated with very low intensity bursts. At the same time the observational signs that determine the ability of AR to cause the eruption of matter from AR into the high layers of the solar corona are still not clear. This makes it difficult for us to understand the eruption initiation physical mechanism (CME trigger). The purpose of this work is to search for observational signs of the onset of eruptive process. For this, we conducted a comparative analysis of pre-flare and flare conditions for flare events, accompanied by CME, and events not accompanied by CME. We studied the features of the spatial dynamics of the microwave and ultraviolet emission (data from the Nobeyama Radioheliograph and SDO/AIA) of AR for selected events.
Interplanetary Coronal Mass Ejections (ICMEs) are among the main drivers of Space Weather and are responsible for the strongest variations in the near-Earth solar-wind conditions. Forecasting the Time of Arrival and Speed of Arrival of an ICME more than an hour ahead is a rather complicated task, since it means propagating a poorly determined plasma and magnetic field structure into an essentially undetermined interplanetary environment.
The Drag-Based Model, despite its simplicity, is still among the most used models to simulate the propagation of an ICME in the heliosphere.
To model the interaction of the ICME with the background solar wind it uses the parameter γ, which is the parameter that modulates the coupling between the solar wind fluid and the ICME body.
Since this parameter incorporates much of the physics of the ICME-wind interaction and its precise value is poorly understood, we think it deserves further investigation.
We built a database with a large number of ICMEs to create a new empirical Probability Distribution Function for γ and to find a suitable functional form to model it.
The determination of solar wind outflow velocity is fundamental to probe the mechanisms of wind acceleration in the corona. Using the Doppler dimming technique, we studied the effects that the chromospheric Lyα line profile shape causes on the determination of the outflow speed of coronal HI atoms. Starting from UV observations (SOHO/UVCS) of the coronal Lyα line and simultaneous measurements of pB (LASCO/SOHO and Mk3/MLSO), we analysed the impact of the pumping chromospheric Lyα line profile through measurements from SOHO/SUMER, UVSP/SMM and LPSP/OSO-8, taken from representative on-disk regions and as a function of time during the solar activity cycle. In particular, we considered the effect of four chromospheric line parameters: line width, depth of the central reversal, asymmetry and distance of the peaks. We find that the range of variability of these parameters is of about 50% for the width, 69% for the depth of the central reversal, 15% for the asymmetry, and 50% for the distance of the peaks. We derive that the variability of the pumping Lyα profile affects the estimates of the coronal HI velocity by about 5-10%. Therefore, this uncertainty is smaller than other physical quantities uncertainties, and a constant in time and unique shape of the Lyα profile over the solar disk can be adopted to estimate the solar wind outflow velocity.
We analyze the measurements of the solar diameter made at the Basilica of San Petronio (Bologna, Italy) from 1655 to 1736 using a meridian line. This series includes the Maunder Minimum, a period of abnormally low solar activity between 1645 and 1715. Some authors have suggested an increase of the solar diameter during the Maunder Minimum. We have applied statistical analyses to compare the solar diameter measured at San Petronio during the Maunder Minimum (1655–1715) and that in a subsequent period (1716–1736). No statistically significant differences are found in the medians and averages of the solar diameter in both periods. In fact, we have found differences around 0.6ʺ, which are below the mean accuracy of the instrument. Therefore, we conclude that there is no difference between the solar diameter value measured during the Maunder Minimum (1655–1715) and that for the subsequent period (1716–1736).
A pair of off-limb eruptions was observed by the Extreme Ultraviolet Imager (EUI) onboard Solar Orbiter (SolO) on 2021 April 23/24. At the time, the spacecraft was at 0.87 AU from the Sun. As seen from Earth, SolO was roughly near the Sun’s east limb (as seen from the Earth) and in quadrature with Parker Solar Probe (PSP), which was at the Sun’s far side. The eruptions are remarkably well observed in the Full Sun Imager (FSI) in both its EUI/FSI174 and EUI/FSI304 channels. The first eruption starts as a slowly growing prominence eruption culminating in an apparent untwisting and ejection from April 23 22:25 UTC onwards. This eruption is immediately followed by a yet more spectacular and faster eruption from the same source region less than 4 hours later. The absence of any corresponding signature in Earth-bound datasets confirms this eruption pair is back-sided from the Earth. STEREO-A COR2 observations confirm that the prominence eruptions observed by EUI/FSI correspond to a complicated interaction of 2-3 coronal mass ejections. In this paper we will use the favourable quadrature orientation of SolO and PSP to link SolO's extreme ultraviolet and coronagraphic observations with PSP's off-limb and in-situ observations. We will highlight the lessons learned for upcoming PSP and Solar Orbiter quadratures such as in February 2022.
We implemented multiple data analysis and machine learning algorithms to extract information of solar active regions that can be used in the future to perform CME and flare forecasting.
We use the data set produced by Angryk et al. (Sci.Data,2020) containing 51 magnetic field parameters and the associated X-ray activity of solar active regions from 2010 to 2018. We performed a data reduction by eliminating redundant parameters in each entry. The reduction was performed using a combination of Common Factor Analysis (CFA) and Principal Component Analysis (PCA). This reduced the mount of data to 5 parameters. To increase the separability of different types of active regions we projected all the points to a 7-dimensional manifold using Sparse Autoencoders (SAE). We then performed supervised and unsupervised classifications of the reduced parameters of each active region. We demonstrate that it is possible to differentiate flaring from non-flaring active regions. We also show that there are tenuous differences between active regions with different flaring activity. However, the current data is not sparse enough to allow a clear differentiation between the different levels of flare activity.
We propose an alternative parametrization of solar active regions. Using Disentangled Variational Autoencoders (beta-VAE) we produce a different representation of the active regions which can be used for classification. We show that this method can be used also to create new unseen artificial active regions to study the evolution of flaring activity, or to solve the problem of data imbalance.
Solar flares are powered by the evolution of the magnetic field, but it is still impossible to deterministically predict whether an active region will flare or not solely based on photospheric information. Observational case studies of the upper solar atmosphere reveal increased levels of magnetic reorganization, dynamics, and temperature variation prior to solar flares. Whether such signatures play a physical role in event initiation, and therefore could improve flare prediction, is still unclear. To this aim, we statistically analyze the coronal and chromospheric conditions prior to solar flares and during flare-quiet periods using data from the Atmospheric Imaging Assembly (AIA) onboard the Solar Dynamics Observatory. AIA Active Region Patches (AARPs), region-targeted extractions of AIA time-series data in (extreme-) ultraviolet are matched to the HMI Active Region Patches (HARPs) for 2010-2018. Pre-event dynamics and heating is parametrized with high-order moment summaries of brightness and running-difference images, plus emission measure, temperature, and density images; temporal behavior is captured by sampling each parameter over a 7hr time-series. NorthWest Research Associates’ Classification Infrastructure (NCI), a well-established statistical classifier system based on Non-Parametric Discriminant Analysis is used to statistically evaluate whether parameters describing the upper atmosphere differ significantly between flaring-imminent vs. flare-quiet populations. Preliminary results and their physical implications will be presented. AARPs are constructed daily, from 15:48-21:48 UT (13 min intervals each hour, time cadence 72s) and will be freely available with this study's publication at www.nwra.com/AARP. This work is supported by NASA Grant HGI/80NSSC19K0285.
Solar flares have direct consequences on the Earth’s ionosphere. The enhancement of extreme ultraviolet (EUV) and X-ray emission during a flare results in the rapid increase of ionization on the entire dayside ionosphere causing a sudden ionospheric disturbance (SID). While SIDs occur in all regions of the ionosphere, the effect on the lowest-lying D-region (60-100km in altitude) is the most apparent. In particular, X-rays with wavelengths < 10 angstroms penetrate down to D-region altitudes and dominate photoionization of all neutral constituents there. This can cause substantial electron density increases in the lower ionosphere to extents large enough to affect the propagation of radio waves used in high-frequency radio telecommunications. Here, by using a combination of solar flare multi-wavelength observations (X-ray and EUV) together with remote sensing of the ionospheric conditions using very low frequency (VLF: 3-30kHz) radio wave propagation, we probe the geophysical effects of flare emission. This work presents a statistical study of flares from the past solar cycle and their impacts on the ionospheric D-region electron density. We look at the relationship between the incident X-ray flux and the D-region response including amplitude variations, heliographic position of flare, relative time-delay analysis and select several events to further investigate the spectral components of a flare and their geophysical impact. We will also discuss the opportunities looking towards solar cycle 25 with both ground-based remote sensing observations of the ionospheric conditions that can be combined with newly available space-based solar which can be utilized in future studies.
The outer atmosphere of the Sun, the corona is comprised of tenuous, highly ionized plasma, that is governed by magnetic fields and is heated to more than a million Kelvin. Such hot coronal plasma is thought to be powered by numerous impulsive heating events called nanoflares. What drives these impulsive nanoflares? What role does magnetic field play in coronal heating? We address these long-standing questions through multi-wavelength observations of the Sun that span from the photosphere through the corona. In this talk, we will present new results that reveal an intricate link between the impulsive coronal heating and the evolution of magnetic fields at the solar surface. In particular, we will discuss the role of magnetic reconnection, a process through which magnetic energy is liberated, in the heating of the solar corona.
At 3.8°, the field of view (FOV) of the Full Sun Imager (FSI) on Solar Orbiter is by far wider than that of any previous solar EUV imager. Depending on the distance of the probe to the Sun along its orbit, this corresponds to 14 to 4 solar radii, to be compared to the 3.5 Rs of STEREO/EUVI or Proba2/SWAP. This very large field of view opens up a new discovery space into a region largely unexplored in the EUV. Since it was expected that stray-light would dominate beyond 2 Rs, a moveable occulting disk can be inserted in the optical path to block light rays up to 0.78° off the optical axis. On March 21 2021, at 0.51 AU, FSI acquired deep exposures at 17.4 and 30.4 nm with the occulting disk in place. The data reveals solar structures extending up to 5 Rs which, to our knowledge, is the furthest ever recorded at these wavelengths. We compare the morphology of the observed structures with close in time observations in white light by the Metis coronagraph. We present a comparison of the measured signal fall-off as a function of distance to Sun-center with a model of coronal emission taking into account collisional excitation and resonant scattering.
Small scale vortices in the solar atmosphere have received increasing attention in recent years. They are ubiquitous at photospheric and chromospheric levels and are a viable candidate mechanism for the exchange of waves, energy, and mass with the upper solar atmosphere.
In order to identify and study the dynamics of these vortices, we seek a suitable mathematical criterion for which an evolution equation exists. The vorticity and vorticity equation would be the classical options for this task. However, it is now well known that they can be biased by shear flows. Therefore, we adopt the swirling strength criterion, a generalisation of the vorticity, for which we derived an evolution equation from the basic equations of (magneto)hydrodynamics. We suggest the swirling strength and its dynamical equation as a novel tool for the analysis of vortex dynamics in numerical simulations.
We apply this novel tool to realistic numerical simulations of a small portion of the solar atmosphere realized with the radiative magnetohydrodynamic code CO5BOLD. We find a tight relation between unidirectional, vertical swirling motions and torsional magnetic field perturbations, which propagate upward at local Alfvén speed and are driven by magnetic tension forces. All together, these are clear characteristics of torsional Alfvén waves in the form of compact wave-packets or unidirectional pulses. These pulses naturally arise from a self-consistent numerical simulation of the solar atmosphere and we estimated the mean Poynting flux at the bottom of the chromosphere.
MHD avalanches involve small, intensely localized instabilities that spread across neighbouring regions in a magnetic field.
Cumulatively, many small events release vast amounts of stored magnetic energy.
Straight cylindrical flux tubes, in Parker (1972)'s model of coronal loops, are liable to such avalanches: one unstable flux tube can cause instability to proliferate through reconnection, resulting in an ongoing chain of like events.
True coronal loops are curved, arching between different footpoints on one photospheric plane.
Using three-dimensional MHD simulations, we here verify the viability of MHD avalanches within the curved magnetic geometry of a multi-threaded coronal arcade.
In contrast to the behaviour of straight cylindrical models, a kink mode occurs more readily and preferentially upwards in this new geometry.
Such instability spreads over a region wider than the original flux tubes, and arguably wider than is seen in a model of straight flux tubes.
Consequently, the release of substantial amounts of energy is sustained, in a series of nanoflare-type events, contributing significantly to coronal heating.
Overwhelmingly, viscous heating dominates over Ohmic, attributable to the shocks and jets produced around these small events.
Reconnection is not the greatest contributor to heating, but rather the facilitator of those processes that are.
Localized and intermittent, the heating shows no strong spatial preference, except for a small bias away from footpoints.
Effects of realistic plasma parameters, and the implications for one-dimensional, loop-aligned models of energetic transport, are discussed.
Parker Solar Probe (PSP) and Solar orbiter have made a number of important discoveries in its exploration of the inner heliosphere/outer corona. Their observation of ubiquitous large amplitude Alfvénic fluctuations, regardless of solar wind speed, in all wind streams except for narrow areas surrounding the heliospheric current sheet, together with large s-shaped inversions of the magnetic field, called switchbacks, begin to call into questions standard ideas of solar wind acceleration. Initial Parker Solar Probe results have shown that slow Alfvénic solar wind intervals appear to be a frequent, if not standard, component of the nascent solar wind inside 0.5 AU. In addition to the strong presence of Alfvénic fluctuations propagating away from the Sun, such intervals also display the huge oscillations - switchbacks, where the Alfvénic fluctuation is accompanied by a fold in the radial magnetic field and a corresponding forward propagating radial jet. Switchbacks often come in patches, separated by short intervals depleted with fluctuations, and periods without switchbacks may also show a striking quiescence, with the magnetic field remaining mostly radial and very small amplitude velocity and magnetic field fluctuations. These observations pose a series of questions on the origins of the solar wind and the role of coronal structure, as well as of the evolution of fluctuations within the solar wind. Here we discuss how the sources of the solar wind measured in situ are related to photospheric and solar magnetic network structures.
Spectroscopy of active regions reveals details of physical processes through measurement of a variety of plasma parameters. The Hinode EUV Imaging spectrometer (EIS) and the NASA IRIS instruments continue to provide spectroscopy from the chromosphere through to the corona. In 2020 the Solar Orbiter mission launched with the SPICE spectrometer onboard. Plans are well underway for a new spectrometer on the next Japanese solar mission, Solar-C. In this review, we will look at results on the behaviour of active regions in non-flaring states and in the build-up to flares. Plasma diagnostics have been used to probe how the active regions loops stay hot and how the flows seen at the edges of active regions can contribute to the slow solar wind - and indeed create energetic particles. In the pre-flare phase, measurements have been made that indicate an increase in non-thermal velocity before the flare begins. We discuss these results and look towards the future of coronal spectroscopy.
On 2011 July 6 EUV channels of AIA instrument onboard SDO detected a recurrent, arc-shaped intensity disturbance over an active region. The intensity disturbance fronts were observed to propagate along a coronal loop bundle rooted in a small area of the dark umbra of the sunspot. Neither signatures of flare activity nor of a coronal mass ejection event were observed in association with the phenomenon. Analysis of EUV wavelengths reveals that the fronts are accelerated in 171 Å and propagate with a projected, averaged plane-of-sky phase velocity of about 60 km/s while for the other coronal channels the values are about 40 km/s. All the channels exhibit a periodic recurrence with a period of about 3 minutes in the umbra and longer periods towards the penumbra. To shed light on the physical nature of the event, we perform 2D numerical simulations based on a simple symmetrical potential magnetic field configuration embedded in a gravitationally stratified atmosphere in hydrostatic equilibrium. We perturb the atmosphere using a driver located below the photosphere with a period of 3 min. We compare the kinematical properties of the event as observed at the different temperature regimes covered by the SDO/AIA images with the results from the numerical simulations. The speed values obtained from numerical simulations are similar to those estimated from observations for 171 Å. The analysis suggests that the accelerated profile seen on 171 Å is due to a projection effect and responds to the slow magnetoacoustic propagating wave scenario.
We studied the kink instability of triangular jets sandwiched between magnetic tubes/slabs and its possible connection to observed properties of the jets in the solar atmosphere. A dispersion equation governing the kink perturbations is obtained through matching of analytical solutions at the jet boundaries. The equation is solved analytically and numerically for different parameters of jets and surrounding plasma. The analytical solution is accompanied by a numerical simulation of fully nonlinear MHD equations for a particular situation of solar type II spicules. MHD triangular jets are unstable to the dynamic kink instability depending on the Alfven Mach number (the ratio of flow to Alfven speeds) and the ratio of internal and external densities. Jets with an angle to the ambient magnetic field have much lower thresholds of instability than field-aligned flows. Growth times of the kink instability are estimated as 6-15 min for type I spicules and 5-60 s for type II spicules matching with their observed life times. Numerical simulation of full nonlinear equations shows that the transverse kink pulse locally destroys the jet in less than a minute in the conditions of type II spicules. Dynamic kink instability may lead to full breakdown of MHD flows and consequently to observed disappearance of spicules in the solar atmosphere.
Magnetic Bright Points (MBPs) are small-scale solar atmospheric structures of highly concentrated magnetic fields that can be studied in ever more details thanks to current high precision measurements and a strong theoretical framework greatly supported by Magnetohydrodynamic (MHD) simulations and its analysis. In this study, we consider a large dataset taken from the HINODE mission from two consecutive solar atmospheric layers and analyze how MBPs evolve over time. We developed new computational techniques to track these small-scale structures and reconstruct their behavior during their lifetime. We found direct evidence for MHD wavelike disturbances within the evolution of their movement paths. We interprete these detected signatures within the MBP tracks as Kink and Sausage wave contributions which can effectively transport energy into the higher atmosphere and thus shedding light on how energy can be transferred throughout the solar atmosphere via the help of flux tubes as wave guides.
Solar wind electrons exhibit complex electron velocity distribution functions (VDFs) shaped by expansion, Coulomb collisions, and field-particle interactions. We investigate how the suprathermal electron deficit in the anti-strahl direction, which was recently discovered in the near-Sun solar wind, drives a kinetic instability and creates whistler waves with wave vectors that are quasi-parallel to the direction of the background magnetic field.
Our study is based on high-cadence measurements of electron pitch-angle distribution functions combined with measurements of electromagnetic waves provided by Solar Orbiter during its first orbit.
The suprathermal electron deficit creates kinetic conditions under which the quasi-parallel whistler wave is driven unstable. We directly test our predictions for the existence of these waves through solar wind observations. We find whistler waves that are quasi-parallel and almost circularly polarised, propagating away from the Sun, coinciding with a pronounced suprathermal electron deficit in the electron VDF. The cyclotron-resonance condition is fulfilled for electrons moving in the direction opposite to the direction of wave propagation, with energies corresponding to those associated with the suprathermal electron deficit.
We conclude that the suprathermal electron deficit acts as a source of quasi-parallel whistler waves in the solar wind. The quasilinear diffusion of the resonant electrons tends to fill the deficit, leading to a reduction in the total electron heat flux.
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It is well established that the total solar irradiance (TSI) varies on
timescales of minute to centuries. On timescales of minutes to hours
the TSI varies due to the globally-averaged superposition of solar
turbulent convection and oscillations, while on solar-cycle and
solar-rotation timescales the majority of the TSI-amplitude
fluctuations are the result of opposing brightenings caused by
faculae/plages and shorter-duration dimmings caused by sunspots. While
TSI variations from minutes to a few decades have been continuously
monitored from space since the late 1970s, TSI variations over much
longer periods of time can only be estimated using either historical
observations of solar surface magnetic features, namely sunspots and
plages, possibly supported by surface flux transport models, or from
the measurements of the cosmogenic isotope (i.e., 14C and 10Be)
concentrations in tree rings and ice cores.
In this work we present a new approach to reconstruct the TSI
variability from the pre-industrial era to the present using component
analysis of time series of historical observations of plages and
sunspots, and the secular trend of the solar potential modulation.
The solar photosphere is characterized by the presence of several structures being sunspots the most visible manifestation of the magnetic field immersed in the convective plasma. The study of such active regions in the photosphere includes the analysis of formation, growth and decay of sunspots. These evolutionary processes are directly related to phenomena of solar activity occurring at upper atmospheric layers. High-resolution solar observations have made it possible to study in detail the dynamics of the solar plasma at different spatial and temporal scales, in particular, through time series of images. Sheeley (1969) first reported radial high-speed flows in the convective pattern around sunspots and called it "moat flow". The study of the moat flow origin is crucial to understand its connections with the structure of the sunspot, for example, the penumbra and their different evolutionary stages. Previous studies have reported links between the moat flow, the Evershed flow and small-scale magnetic elements called Moving Magnetic Features (MMFs). In this work, local correlation tracking techniques are employed over time series of solar images acquired with the Solar Dynamics Observatory in the continuum, in order to study proper motions in the plasma granular pattern in the vicinity of sunspots during the decaying phase and characterize the endmost evolution of plasma flows in the active regions.
Magnetic field vector observations in the solar photosphere have generally revealed a non-zero value of the divergence: the vertical field component gradient is found on the order of 3 G/km when the horizontal field component gradient is of 0.3 G/km only. This has first to be assigned to the fact that the measured quantity is the magnetic field H, which is related to the divergence-free magnetic induction B by the law B=µ0(H+M), where M is the magnetization. In plasmas like the solar photosphere, magnetization results from plasma diamagnetism and spiral movement of charged particles about the magnetic field. It can be observed that in the solar interior the electron thermal velocity is much larger than the escape velocity from both gravity and proton attraction. A model of this is presented in the related paper (Bommier, V., "Solar photosphere magnetization", 2020, A&A, 634, A40). The electrons escape from lower layers in a quasi-static spreading, and accumulate in the photosphere. Therefore, the electron density at surface is increased but decreases with height at surface, which enables the observed values because divH = -divM. Such a structure is probably at play in the solar-type stars. Besides, solar magnetohydrodynamics must include the fact that the quantity measured by Zeeman effect is H (4 demonstrations in the paper), which is related to the electric current j by the Maxwell relation rotH = j, where j is itself submitted to the Lorentz force j x B, where B is the divergence-free magnetic induction.
A large-scale magnetic cycle is possible in the Sun and other stars as long as the large-scale shear and helicity of the plasma flow in their convection zones are sufficiently strong. Hence, there is a critical dynamo number for each star for the operation of a large-scale dynamo. As a star spins down, it is expected that the large-scale dynamo ceases to operate above a critical rotation period. Our study explores the possibility of the operation of the dynamo in the subcritical region using the Babcock-Leighton type kinematic dynamo model. In some parameter regimes, we find that the dynamo shows hysteresis behavior, i.e., two dynamo solutions are possible depending on the initial parameters---decaying solution if started with weak field and strong oscillatory solution (subcritical dynamo) when started with a strong field. However, under large fluctuations in the dynamo parameter, the subcritical dynamo mode is unstable in some parameter regimes. Therefore, our study supports the possible existence of subcritical dynamo in some stars which was previously shown in a mean-field dynamo model with distributed $\alpha$ and MHD turbulent dynamo simulations.
The Babcock-Leighton (BL) mechanism, in which the poloidal field is produced by the emergence and subsequent dispersal of sunspot groups, has been received more and more observational evidence during the past decade. Most BL-type dynamo models assume that the toroidal field is generated in the tachocline. However, recently the importance of the tachocline has been questioned by magnetic activity of fully convective stars. We aim to develop a new generation of BL-type dynamo model, in which the dynamo operates mainly within the convection zone. We introduce the near-surface turbulent pumping into the BL-type dynamo model with a vertical upper boundary condition. Other ingredients include solar-like internal differential rotation, a single-cell meridional flow with penetration depth of 0.7R, and the magnetic diffusivity of $5.0\times10^{11}cm^{2}s^{-1}$. The pumping causes the poloidal field within the convection zone to be almost in the purely latitudinal direction. Due to the latitude shear in the bulk of the convection zone, most of the toroidal field is generated there. Our model reproduces the basic properties of the solar cycle, including a) 22 years magnetic cycle; b) equatorward propagation of the activity belts; and c) phase difference between the activity belts and polar field. The results do not depend on the existence of the tachocline or not. The near-surface pumping enhances the coupling of the poloidal field between the northern and southern hemispheres to reproduce solar-like dipolar parity.
The solar dipole moment at cycle minimum is considered to be the most reliable precursor to determine the amplitude of the subsequent cycle. Numerical simulations of the surface flux transport (SFT) model are widely used to effectively predict the dipole moment. An algebraic method was recently proposed to quickly predict the contribution of an active region (AR) to the axial dipole moment at cycle minimum instead of SFT simulations. The method assumes a bipolar magnetic region (BMR) configuration of ARs, however most ARs are asymmetric in configuration of opposite polarities, or have more complex configurations. Such ARs evolve significantly differently from those of BMR approximations. We propose a generalized algebraic method to describe the axial dipole contribution of an AR with an arbitrary configuration, and evaluate its effectiveness compared to the BMR-based method by comparing its results with SFT simulations of observed ARs and artificial ARs. We also compare the results with those from the BMR-based method. The generalized method is equivalent to the SFT model, and precisely predicts the contributions of ARs to the dipole moment, but has a much higher computational efficiency. Although the BMR-based method has similar computational efficiency to the generalized method, it is only accurate for symmetric bipolar ARs. The BMR-based method systematically overestimates the dipole contributions of asymmetric bipolar ARs, and randomly miscalculates the contributions of more complex ARs. The generalized method quick and precisely quantifies an AR's contribution to solar cycle evolution, which paves the way for application in physics-based solar cycle predictions.
We investigate a new method to obtain the plasma parameters of solar prominences observed in the Mg II h&k spectral lines by comparing line profiles from the IRIS satellite to a bank of profiles computed with a one-dimensional non-LTE radiative transfer code. The prominence observations were carried out by the IRIS satellite on 19th April 2018. Using a grid of 1007 one-dimensional non-LTE radiative transfer models, some including a prominence-corona transition region (PCTR), we are able to recover satisfactory matches in areas of the prominence where single-line profiles are observed. Large values of ionization degree are found by the procedure in areas where the line of sight crosses mostly plasma from the PCTR, correlating with high mean temperatures and correspondingly no Hα emission. The models were unable to recover satisfactory fits in the regions where we see Hα emission. This is due to the complex line shapes manifesting from many unresolved independently moving threads. This issue might be solved in future by increasing the microturbulent velocities in the models to simulate these unresolved movements.
This new method naturally returns information on how closely the observed and computed profiles match, allowing the user to identify areas where no satisfactory match between models and observations can be obtained. The inclusion of the PCTR was found to be important, as regions where satisfactory fits were found were more likely to contain a model encompassing a PCTR.
We report on diagnostics of the off-limb solar corona using coordinated observations of EUV allowed lines together with the coronal forbidden lines. We show that the electron densities obtained from the Fe XIII line ratios observed by both Hinode/EIS and COMP are in good agreement once the photoexcitation and background subtraction are both accounted for. In addition, the Hinode/EIS observations of Fe XII indicate that the 195.1 A line has an anomalous width and is likely optically thick. The Fe XII 1349 A forbidden line observed by IRIS shows enhanced intensities in the active region spectra, but not in the quiet Sun. These observations can be explained by presence of high-energy electrons in active region corona.
Ellerman Bomb-like brightenings of the hydrogen Balmer line wings in the quiet Sun, also known as quiet Sun Ellerman bombs (QSEBs), are a signature of the fundamental process of magnetic reconnection at the smallest observable scale in the lower solar atmosphere. We analyze high spatial resolution observations (0.″1) obtained with the Swedish 1-m Solar Telescope to explore signatures of QSEBs in the Hβ line. We find that QSEBs are ubiquitous and uniformly distributed throughout the quiet Sun, predominantly occurring in intergranular lanes. We find up to 120 QSEBs in the field of view for a single moment in time; this is more than an order of magnitude higher than the number of QSEBs found in earlier Hα observations. This suggests that about half a million QSEBs could be present in the lower solar atmosphere at any given time. The QSEB brightenings found in the Hβ line wings also persist in the line core with a temporal delay and spatial offset toward the nearest solar limb. The observed QSEBs vary significantly in their properties, such as lifetime, brightness, and size. Our results suggest that QSEBs emanate through magnetic reconnection along vertically extended current sheets in the lower solar atmosphere. The apparent omnipresence of small-scale magnetic reconnection may play an important role in the energy balance of the solar chromosphere.
Analysis of the dynamics of the hot coronal plasma is the most promising method
to examine the contribution of wave-like phenomena in the global heating of the solar corona.
We present here a new, state-of-the art instrument for imaging spectroscopy:
the Solar Line Emission Dopplerometer (SLED). It is based on the Multi-channel
Subtractive Double Pass (MSDP) principle, which combines the advantages of
filters and slit spectrographs. The SLED (presently under construction) will observe
coronal structures in the forbidden lines of FeX 637.4 nm and FeXIV 530.3 nm. It will
measure Doppler shifts up to 150 km/s with high precision (50 m/s) and fast cadence (1 Hz),
over a 1000" x 150" rectangular FOV (for six meter telescope’s focal length).
The SLED is optimized to detect high-frequency wave-like plasma motions
which could be the signatures of the coronal heating processes and allows
studies of the dynamics of fast evolving events. A numerical simulation of
observations is shown to demonstrate the capabilities of the instrument.
The regular observations will be performed with the high-altitude coronagraph
at Lomnicky Stit Observatory (LSO), and during total solar eclipses.
A joint campaign of various space-borne and ground-based observatories, comprising the Hinode-SOT, IRIS, EIS (HOP 381, 10 – 22 October 2019), and the GREGOR Solar Telescope, investigated Quiet Sun regions for inferring the plasma β at photosphere, transition region, and corona. This campaign provided co-spatial and co-temporal observations, which can provide values of the magnetic field, temperature, and density in the solar atmosphere. They can help us to complete a more detailed depiction of the plasma β with height. We present the preliminary results of coordinated multiwavelength observations. Temperature estimates in the photosphere were obtained using High-resolution Fast Imager (HIFI at GREGOR) in blue continuum and G-band wavelengths. In the transition region, density diagnostics were obtained through the emissivity ratio method on OIV and SIV lines of the Interface Region Imaging Spectrograph (IRIS). Finally, coronal density estimates were derived from the line pair Fe XII 186/195 of the Extreme-ultraviolet Imaging Spectrometer (Hinode-EIS) and coronal temperatures from differential emission measure (DEM) using Atmospheric Imaging Assembly (AIA-SDO) datasets.
Solar flares are generally thought to be the impulsive release of magnetic energy giving rise to a wide range of solar phenomena that influence the heliosphere and in some cases even conditions on Earth. Part of this liberated energy is used for particle acceleration and to heat up the solar plasma. The Spectrometer/Telescope for Imaging X-rays (STIX) instrument onboard the Solar Orbiter mission promises considerable advances in the understanding of electron acceleration and plasma heating. It observes X-rays in the energy range from 4 to 150 keV, enabling it to diagnose thermal plasma with temperatures of ≳ 10 MK, as well as nonthermal bremsstrahlung emission of flare accelerated electrons. During the spacecraft commissioning phase in 2020, STIX observed 68 microflares, all of which originated in an active region that was also visible from Earth. These events provided a great opportunity to demonstrate the great potential in combining the STIX observations with multi-band EUV imagery from the Atmospheric Imaging Assembly (AIA) instrument on board the Earth orbiting Solar Dynamics Observatory.
We show first results from two GOES B-class events for which we combined STIX spectroscopic analysis with plasma diagnostics through differential emission measure analysis performed on AIA observations to analyze thermal flare plasma outside STIX’s sensitivity. We find that the thermal parameters inferred from STIX and AIA differ due to the different temperature ranges covered by each instrument. The values deduced from STIX are consistent with similar sized flares in the literature. We conclude that STIX spectroscopy is science ready.
Condensations are observed in many astrophysical environments. In solar physics, common phenomena are coronal rain and prominences. Coronal rain consists of transient dense blobs that form in magnetic loops and rain down along the magnetic field lines. The prominences are cold, dense structures suspended in the hot, tenuous corona by the magnetic field.
Those structures are formed due to energy loss via optically thin radiative emission. Instead of solving the full radiative transfer equations, precomputed cooling curves are typically used in multidimensional, magnetohydrodynamic (MHD) simulations assuming an optically thin and fully ionised plasma. Precomputed cooling curves used in literature differ greatly, depending on the incorporated plasma emission processes, atomic physics data, and solar abundances.
We study the effect of the optically thin cooling curves on the formation and evolution of condensations. The condensations are formed due to thermal instability. We use the open-source software MPI-AMRVAC to setup idealised simulations, i.e. a thermal equilibrium in a 2D local coronal volume perturbed by interacting slow MHD waves. For all cooling curves, condensations are formed by thermal instability. However, the differences are twofold. First, the growth rates of the thermal instability are different, leading to condensations being formed at different times. Second, the morphology of the condensations is widely varying. This is influenced by the low-temperature treatment of the cooling curves. Furthermore, we discuss a bootstrap procedure that allows us to continue high-resolution simulations of thermal instability far into the nonlinear regime.
Computing synthetic spectra from model atmospheres is a fundamental tool to understand the formation of complex spectra and help guide observations. Forward modelling using 3D MHD simulations is becoming widespread, and with it the need to efficiently carry out radiative transfer computations. This is particularly acute for the solar chromosphere, where out of equilibrium conditions dictate the need for non-LTE calculations, which in 3D are computationally extremely expensive and require a supercomputer. We have developed a neural network approach to greatly speed up 3D non-LTE spectral synthesis. We used a convolutional neural network to learn the full 3D mapping between LTE and non-LTE populations for a given model atom. Once we have the non-LTE populations, synthetic spectra can be quickly computed for any viewing angle and spectral line, assuming complete redistribution (CRD). The ``true'' values of the non-LTE populations are taken from runs with the Multi3D code. The proposed network architecture successfully learns the population mappings using a combination of simulations with different conditions and magnetic topology. Testing with different snapshots of the simulations used in the training gives a very good agreement, although the network can struggle when using more extreme, out of sample simulations. The results are very encouraging and result on a time saving of about 5 orders of magnitude; running typical-sized problems for a model hydrogen atom takes less than three hours on a consumer GPU.
In the corona, the (apparent) thermal equilibrium arises from a delicate balance between radiative losses and some unknown heating mechanism(s). The effect of these heating and cooling mechanisms varies with the plasma parameters, such as density, temperature and potentially magnetic field strength. Meanwhile, slow magnetoacoustic waves can perturb the density and temperature of the hosting plasma enough to affect these heating and cooling mechanisms, to the extent that the waves themselves are impacted in a measurable way. Thus there is great potential in exploiting these slow waves, which are commonplace in the corona, as probes of the local thermal equilibrium.
In this talk I will outline how, by measuring the properties of slow waves as they perturb the coronal equilibrium, we may place some constraints on the poorly understood coronal heating function. I will show that if the magnetic field is sufficiently strong, even if the heating mechanism depends strongly on magnetic field strength, the slow waves are insensitive to this (magnetic) dependence. This holds true in the corona so long as the magnetic field strength is greater than approximately 10G for quiescent loops and plumes, and 100G for hot and dense loops.
We aimed to study the damping mechanism of the large-amplitude longitudinal oscillations (LALOs) in solar prominences hidden by numerical dissipation. We performed the numerical simulations of LALOs using the 2D magnetic configuration that contains the dipped region. After the prominence mass loading in the magnetic dips, we triggered LALOs perturbing the prominence mass along the magnetic field. We used the same numerical setup gradually increasing spatial resolution. We obtained a good agreement of the period of LALOs with the pendulum model for the simulation with the highest spatial resolution. The analysis of motions revealed that the damping time is similar in the two experiments with the finest grid-scale, indicating that the further improvement of the spatial resolution does not change the damping time of LALOs in the central and bottom prominence region. This indicates that the physical mechanism is responsible for the attenuation of LALOs in those prominence regions. At the prominence top, the oscillations are amplified in the first minutes and then slowly attenuated. The characteristic time suggests more significant amplification in the experiments with high spatial resolution. We have found that energy losses at the bottom prominence region are caused by wave leakage and the energy exchange between the bottom and top prominence regions. We concluded that the high-resolution simulations are crucial for studying the periods and the damping mechanism of LALOs. Furthermore, numerical diffusion can hide the important physical mechanisms as the amplification of oscillations.
We aim at setting and driving 3D magneto-hydrodynamic simulations of the Sun with photospheric magnetogram observations to get a better understanding of the heating mechanism and energy dissipation in the solar corona and thus aiming to move a step closer towards the long-standing solar coronal heating problem. There are already some models that study coronal heating using different heating mechanisms. The working mechanism for our model is the field-line braiding mechanism generating an upward Poynting flux, where plasma motions advect the field. This flux travels as magnetic perturbations into the corona indicating actual magnetic-energy transport. These perturbations can then induce electric currents in the solar corona which are then dissipated due to DC heating. We start the computation with an initial atmospheric stratification that is usually not in hydrodynamic equilibrium. Because settling the initial inequilibrium is costly in large-scale 3D models, instead, we use a 1D model that spans from the solar interior to the corona for finding the numerical equilibrium that exactly fits to the simulation parameters. This new atmospheric stratification we can now use as the initial condition for large simulation runs. Also, we implement and employ an artificial heating function that compensates for a lack of heating in the early phase of the model, where perturbations have not yet reached the corona. We like to start the 3D model with the most realistic physics and less vertical settling motions. This procedure finally allows us to compare our model output with actually observed Doppler shifts in the corona.
Despite the recent lull in solar activity, the community has seen new observational discoveries and new advances in the modelling of the umbra. The presence of coronal and transition region downflows have been repeatedly reaffirmed, their role in the typical umbral upper chromosphere remaining unconstrained. A connection between small-scale dynamic fibrils and umbral flashes has been established using semi-empirical inversions that leave open questions regarding the top-most chromospheric temperatures. In parallel ALMA has confirmed the presence of increased radio emission from the chromospheric umbra of unknown source and at unconstrained formation heights. It is not clear how, if at all, these three pieces of the puzzle fit together. We review these advances together as the new open questions were not obvious before. Using synthetic observables from different inversions set in such a way that they lead to the very different models found in the literature, we present how some of the open questions can be answered either in the optical or, even more promisingly, in mm wavelengths. In the process we settle the formation heights for multiple ALMA passbands in the umbra and provide approaches to solve non-LTE inversion degeneracies in the optical. High quality SST data is very briefly presented in the context of dynamic fine-structures and how such features might impact the also recently discovered resonant mode signatures.
Solar prominences are cold, dense structures nested in the hot and tenuous solar corona, made up of thread-like fibrils. Embedded in the magnetically dominated, dynamic corona, prominences also exhibit oscillatory behavior [1]. Understanding the interplay of mechanisms that cause prominence and thread oscillations provides important insight into the solar corona. Numerical simulations have been conducted [2, 3, 4] in order to analyze the exact mechanisms governing prominence behavior. To date, all studies on oscillations in prominences ignored their finer structure. The goal of this work is to study causal relations between a localized energy release and a remote prominence oscillation where the prominence has a realistic thread structure. In our setup, we notice coupled transverse and longitudinal oscillations. We use an adiabatic, 2D numerical model with an open-source MHD simulation code, MPI-AMRVAC [5]. We exploit the advantages of adaptive mesh refinement (AMR) to investigate how multiple threads react to a realistic source perturbation. The grid we employ consists effectively of 4160 × 800 cells, which allows us to resolve lengths of 36×7.5 km. This exceeds the resolution limits of observations.
In order to infer the properties of the coronal plasma, coronal seismology combines the measurement of temporal and spatial signals of oscillations and magnetohydrodynamic waves of different magnetic structures with their theoretical modeling. In the particular case of coronal loops, fast sausage modes and standing slow modes are the most studied oscillation modes, because their compressibility makes them susceptible to being observed. By performing magnetohydrodynamic numerical simulations, we analyze the capability of different types of disturbances, associated with typical solar corona energy fluctuations, to generate these types of modes. We found that confined energy deposition excites slow modes, while global perturbations, capable of instantly modifying the loop temperature, excite fast sausage modes.
In the context of the solar coronal heating problem, one possible explanation for the high coronal temperature is the release of energy by magnetohydrodynamic (MHD) waves. The energy transfer is believed to be possible, among others, by the development of the Kelvin-Helmholtz instability (KHI) in coronal loops. Our aim is to determine if standing slow waves in solar atmospheric structures such as coronal loops, and also prominence threads, sunspots, and pores, can trigger the KHI due to the oscillating shear flow at the structure’s boundary. We used linearized nonstationary MHD to work out an analytical model in a cartesian reference frame. The model describes a compressible plasma near a discontinuous interface separating two regions of homogeneous plasma, each harboring an oscillating velocity field with a constant amplitude which is parallel to the background magnetic field and aligned with the interface. The obtained analytical results were then used to determine the stability of said interface, both in coronal and photospheric conditions. We find that the stability of the interface is determined by a Mathieu equation. In function of the parameters of this equation, the interface can either be stable or unstable. For coronal as well as photospheric conditions, we find that the interface is stable with respect to the KHI. Theoretically, it can, however, be unstable with respect to a parametric resonance instability, although it seems physically unlikely. We conclude that, in this simplified setup, a standing slow wave does not trigger the KHI without the involvement of additional physical processes.
The MANCHA code development was started in 2006 to study wave dynamics in sunspots at the Instituto de Astrofísica de Canarias.
Since then it has gradually been upgraded by adding new physics and improved programming techniques.
The code can be used for a large variety of problems from linear wave propagation and classical hydrodynamic instabilities to highly realistic simulations of convection-driven solar and stellar atmosphere.
The code solves the MHD equations including nonlinear terms for the ambipolar and Hall diffusion, the Ohm's heating and the Biermann battery.
The radiative energy exchange is implemented by the short-characteristics method.
The equation of state is either ideal (computed on the fly) or realistic (interpolated from pre-computed lookup tables provided by the user).
The code uses uniform Cartesian grid with spatial discretization up to 6th order; the Runge-Kutta scheme is used for the time integration.
A super-time-stepping technique is implemented to overcome timestep limitation due to diffusion processes.
Hyper-diffusion and filtering are available to stabilize the high-frequency numerical noise.
A perfectly-matched-layer is implemented as an optional non-reflecting boundary condition.
MANCHA is written in Fortran and parallelized with MPI, including parallel I/O using the HDF library.
In order to solve a new problem, users will need to find their own optimal set of parameters in an input control file.
In the case of non-periodic boundaries, users are expected to create their own boundary condition module.
A set of samples together with the manual provide basic instructions on how to do that.
The absorption coefficients of hydrogen plasma, calculated within the frame of cut-off Coulomb potential model, for the wide area of electron densities and temperatures observed within the solar atmosphere are presented here. The optical parameter of hydrogen plasma of mid and moderately high nonideality parameter could be described successfully, thus enabling the modeling of optical properties, especially the calculation of plasma opacity. The model was proven in both convergence towards normal condition, ideal plasma case, as well as with the help of analysis of the experimental data and further theoretical consideration. The model potential is solvable in entire space and within entire energy spectrum, thus the yielded wave function solutions are a combination of a special functions. The special form of the cut-of Coulomb potential, possesses an unique feature that enables the precise, fully quantum method of calculation of inverse Brehmstrahlung effect. Although the presented method development is still a work in progress the possibility of unifying a mode for both transport and optical properties of plasma within same model is an attractive direction for it’s further development.
We present our findings on MHD wave propagation and instabilities in asymmetric Cartesian waveguide models. Generalising the classical slab models this way, thanks to the introduction of various sources of asymmetry (background density, magnetic field or flow speed) allows us to more precisely investigate several important features in the richly structured solar atmosphere. By developing solar magneto-seismologic methods from these analytical models, we can provide an efficient tool for obtaining further information about the solar plasma from observations. We offer further detail on the types and parameters of MHD waves expected to propagate and be observable in a number of multi-layered systems of the solar atmosphere (such as e.g. magnetic bright points or light walls) with new, high-resolution technology.
The atmosphere of the sun represents a complex physical environment
where two traditional classes of fluid theories come to interplay. While the solar chromosphere is typically modeled with fluid models derived under the highly-collisional assumption, whereas the collisional frequencies in the solar corona can become so small, that collisionless fluid models seem to be more appropriate. We briefly overview these two distinct classes of fluid theories and discuss the major differences between them. We also discuss some preliminary results from a 3rd unifying class of arbitrary-collisional models that are suitable for any regime of collisionality.
The magnetic and current helicity of the field above active regions is thought to play a role when estimating the probability for coronal mass ejections or strong reconnection events. A deeper understanding of the mechanisms generating the helicity in the corona can be obtained with the help of observationally driven models, in particular magneto-hydrodynamic and ambipolar-diffusion simulations. We aim to study where the helicity may decouple from the Sun to be ejected into inter-planetary space. While the handedness of the helicity in the heliosphere was observed to be exactly reversed as in the solar interior, we expect to find the required sign reversal in the helicity somewhere in between. We employ large magneto-hydrodynamic model to investigate the actual helicity above a really observed active region. In addition, we set up small artificial sunspot groups to observe which handedness of helicity is generated due to the geometric configuration and magnetic polarity of the spots. This leads us to a quasi-scalar formulation for the generated helicity above multipolar sunspot configurations. We find that some configurations create a local helicity in the corona that is opposite to the expected handedness at the solar surface. We conclude that such configurations may be more eruptive than others.
Coronal mass ejections (CMEs) are one of the main factors determining space weather. The results of the study of CMEs, type II radio bursts (RBIIs) and CMEs associated with RBIIs (RBII CMEs) observed from 1995 to 2017 are presented.
DH RBIIs are believed to be generated by magnetohydrodynamic shock waves. CMEs are considered to be the main phenomenon of solar activity, which are the sources of these shock waves. The study showed that CMEs associated with RBIIs constitute a separate CME population. CMEs and RBII CMEs behave differently in cycles 23 and 24. While the total number of CMEs increased in cycle 24 compared to cycle 23, the number of RBII CMEs decreased. In cycle 24, not only the number of CMEs increased, but also their parameters and the nature of cycle variations changed. Different types of CMEs behave differently during cycles 23 and 24.
The results indicate that the cycle variations in the number of both CMEs and RBII CMEs, and their parameters do not correspond to the well-known evolution of active regions. The dependence of the rate and parameters of the RBII CMEs and RBIIs on the magnetic field strength and plasma parameters in the solar atmosphere has been revealed. The decrease in both the polar and nonpolar magnetic fields of the Sun observed in cycle 24 led to changes in the coronal and interplanetary plasma, which influenced both the CME parameters and the nature of their propagation, and the conditions for the generation of RBIIs.
We present simultaneous magnetic field measurements for the limb solar flare of 1981 July 17 using of the Ca II K, H$\delta$, He I 4471.5 Å and H$\beta$ lines (Yakovkin et al., 2021; https://doi.org/10.1016/j.asr.2021.03.036). For two moments during the flare, which differ in time by 16 min, we analyzed Stokes $I \pm V$ and $V$ profiles of these lines from observations made on the Echelle spectrograph of the horizontal solar telescope of the Astronomical Observatory of Taras Shevchenko National University of Kiev. For heights of 10$-$18 Mm above the level of the photosphere, we found that (a) very strong kG magnetic fields (up to about 3 kG) existed at both moments of the flare, (b) the locations with strongest fields, in general, do not coincide for different spectral lines, (c) the polarities of the magnetic field for different spectral lines are in most cases identical, but sometimes they do not coincide. The data obtained indicate a significant inhomogeneity of the magnetic field in the flaring corona and the probable presence of the conditions necessary for magnetic reconnection of field lines. A new indication of the existence of superstrong magnetic fields ( > 5 kG ) follows from a comparison of the kinetic temperatures and turbulent velocities in the flare (Yakovkin & Lozitsky, 2020; https://doi.org/10.18524/1810-4215.2020.33.216453). From analysis of Stokes $I$ profiles, we found a tendency to anti-correlation between temperature and turbulent velocity. Perhaps, this unlikely tendency presents masked presence of very strong magnetic fields of 7$-$8 kG range.
Radio zebras are detected as narrow-band stripes in radio observations from Sun, Jupiter, and Crab pulsar. They are Type IV radio fine structures and can help with diagnoses of local plasma properties in the active solar regions. The double plasma resonance model of solar radio zebra assumes dense and cold background isotropic plasma and rare hot component with an unstable loss-cone type of distribution function. The instability generates the Bernstein electrostatic waves that can transform into electromagnetic radiation. We used analytical theory and 3D electromagnetic relativistic Particle-in-Cell simulations and found that increasing the temperature shifts the growth-rate maxima to lower frequencies for the DGH velocity distribution function of hot electrons. Moreover, the maxima are not distinguishable for loss-cone thermal velocities $v_\mathrm{t} \geq 0.3\, c$. We estimated the brightness temperature, energy density, size of the zebra emission source, and conversion rates into electromagnetic waves.
Using data from SDO/HMI, Hinode/SOT, and LYRA instruments, we study the white-light continuum emission during the X9.3 solar flare (SOL2017-09-06T11:53). Assuming that the emission is due to hydrogen Balmer and Paschen continua, we estimate the temperature evolution during that solar flare.
Coronal dimmings are temporary regions of strongly reduced emission in extreme-ultraviolet (EUV) and soft X-rays caused by expansion and evacuation of plasma associated with coronal mass ejections (CMEs).
We seek to gain insight into observed features of coronal dimmings (location, dynamics, intensity distribution) as they relate to magnetic reconnection due to the associated flare. We analyze the X2.1 flare/CME event on September 6, 2011 by combining EUV observations of coronal dimmings from SDO/AIA with MHD simulations initiated by a non-force-free magnetic field extrapolation.
The extrapolation captures a 3D null point configuration overlying a highly sheared arcade, co-spatial with an observed sigmoid in 94Å. Prior to the flare, small but distinctly bipolar dimming regions are observed in 211Å logarithmic base-ratio images. These dimmings likely form due to rising magnetic loops reconnecting at the pre-existing 3D null point; the reconnection leads to the expansion and loss of previously confined plasma.
The simulated dynamics show the transfer of twist from the arcade to the overlying loops through reconnection, forming a flux rope. We find that simultaneous reconnections at the 3D null and an X-type geometry, newly formed between the flux rope and lower-lying arcades, can explain the observed flare ribbons.
Finally, reconnection at the 3D null transforms closed inner spine field lines into open field lines of the outer spine. Footpoints of these field lines appear to trace the dome as they correspond to a ring-shaped dimming region. Plasma loss along open field lines can potentially explain dimming regions of strongest intensity decrease.
The Nancay Radioheliograph is dedicated to imaging the solar corona at decimetre-to-metre wavelengths. The imaged structures are the quiet corona, through thermal bremsstrahlung, and bright collective emissions due to electrons accelerated in quiescent, flaring and eruptive active regions. After more than five years of interruption for an instrument upgrade, solar observations were resumed in November 2020. This contribution will give a brief overview of the technical changes and present observations at eight frequencies of solar activity since November 2020. During the perihelion passages of Parker Solar Probe in January and April 2021 several radio events produced by electron beams (type III bursts) were observed, where the radio imaging provides insight into the coronal regions that guide particles to the interplanetary space. We will illustrate these observations with an attempt to reconstruct the 3D structure of the propagation paths. We will furthermore address more complex radio sources associated with coronal mass ejections and solar energetic particle events.
We present the observations of two type III solar radio events performed with LOFAR (LOw-Frequency ARray) station in Bałdy (PL612), Poland in single mode. The first event occurred on 20th August 2017 and the second one on 9th September 2017. Solar dynamic spectra were recorded in the 10 MHz up to 90 MHz frequency band. Together with the wide frequency bandwidth LOFAR telescope (with single station used) provides also high frequency and high sensitivity observations. Additionally to LOFAR observations, the data recorded by instruments on boards of the Interface Region Imaging Spectrograph (IRIS) and Solar Dynamics Observatory (SDO) in the UV spectral range complement observations in the radio field. Unfortunately, only the radio event from 9th September 2017 was observed by both satellites. Our study shows that the LOFAR single station observations, in combination with observations at other wavelengths can be very useful for better understanding of the environment in which the type III radio events occur.
The Sun cubE onE (SEE) is a proposed 12U CubeSat mission in LEO that will investigate Gamma and X-ray fluxes and UV solar emission to support studies in Sun-Earth interaction and Space Weather. SEE's primary goal is to monitor the emission from soft-X to Gamma ray energy range and the solar activity using full disk images in the Mg II doublet at 280 nm.
The Gamma and X-ray fluxes will be studied with unprecedented temporal resolution and with a multi-wavelength approach thanks to the combined use of silicon photodiode and SiPM based detectors. The flare spectrum will be explored from the KeV to the MeV range of energies by the same payload, and with a cadence > 10 kHz to investigate the sources of the solar flares.
Given its UV imaging capabilities, SEE will be a key space asset to support detailed studies on solar activity, especially in relation to ultraviolet radiation which strongly interacts with the upper layers of the Earth's atmosphere, and in relation to space safety, included in the field of human exploration.
SEE data will be used together with space and ground-based observatories that provide Solar data, high energy particle fluxes and geomagnetic data in a multi-instrument/multi-wavelength/multi-messenger approach. SEE has recently passed the technical assessment by Italian Space Agency and it is currently in the shortlist of mission proposals for which the commission will proceed to the adequacy assestment.
The European Union’s Flare Likelihood and Region Eruption Forecasting (FLARECAST) project ran between January 2015 and February 2018. It comprised the synergistic, interdisciplinary work of tens of researchers active in the fields of solar physics, space weather forecasting, computer science, big data, infrastructure and science communication. The theme of the project was solar flare prediction and its three primary objectives were to, first, understand the drivers of the flare phenomenon and improve flare forecasting, second, provide a globally accessible flare forecast service scalable enough to facilitate expansion and, third, engage with space weather end users, stakeholders and the public in an effort to raise awareness and educate on the need to predict solar flares and space weather, in general. We attempt an overview of the results of accumulating more than 170 apparent flare predictors extracted by photospheric magnetic field measurements over the past solar cycle and using them as input in 14 supervised and unsupervised machine learning forecast methods. We further brief on project-supported modeling works aiming to highlight potentially promising leads toward forecasting and to link flare activity with coronal mass ejections. We also detail on the recent open availability of the project’s data, codes and infrastructure in hopes of avoiding effort duplication in future forecasting efforts. The current state-of-the-art and potentially meaningful actions for the future are also discussed. The project’s overview paper is available in arXiv (2105.05993). Results shown have received support by the EU Horizon 2020 FLARECAST project (grant agreement no. 640216).
The SunDish project is devoted to radio imaging and monitoring of the solar atmosphere at high radio frequencies (at present 18-26 GHz, up to 100 GHz in perspective) through single-dish observations with INAF radio telescopes.
Observations of the brightness temperature of the solar atmosphere in the radio band can map plasma processes that produce free-free emission in the local thermodynamic equilibrium and gyromagnetic phenomena, providing a probe of physical conditions in a wide range of atmospheric layers both for quiet and active regions.
During the development and early science phase of the project (2018-2020), we obtained about 170 maps of the entire solar disk in the 18-26 GHz band, filling the observational gap in the field of chromospheric imaging at these frequencies.
In order to ease the multi-wavelength exploitation of our data products, we present a first catalogue of continuum imaging observations including the multi-wavelength identification of active regions and their brightness and spectral characterization.
Through systematic monitoring of the Sun, our system can provide: (1) accurate measurement of the brightness temperature of the radio-quiet Sun component, that has been poorly explored in the 20-26 GHz range to date; (2) characterization of the flux density, spectral properties and long-term evolution of dynamical features (active regions, coronal holes, loop systems, streamers, and the coronal plateau); (3) prediction of powerful flares through the detection of peculiar spectral variations in the active regions, as a valuable forecasting probe for the Space Weather hazard network.
Solar flare forecasting can be realized by means of either the numerical solution of model equations or the analysis of magnetic data by means of artificial intelligence techniques. Here we consider this second approach and discuss how neural network optimization and forecasting assessment by means of skill scores are deeply intertwined. A special focus is also given to the interpretation of data descriptors in terms of their impact on the prediction effectiveness. Applications will be concerned with magnetograms recorded by SDO/HMI, in the case of both point-in-time images and time series of magnetogram frames.
We examine the characteristics of ULF waves observed in the magnetosphere and at ground on June 23, 2020 during super solar quiet geomagnetic conditions. A highly monochromatic and large-amplitude wave at f = 1.67 mHz was observed between 6:10 and 7:00 UT at CSES LEO satellite orbit and across a wide longitudinal range of ground stations from low to high latitudes. We found the possible driver of such global ULF wave activity in the impact of a Tangential Discontinuity intersecting the bow shock quasi-parallel to it. As a consequence, a foreshock bubble (FB) was generated, producing pressure pulses which in turn generates Pc5 waves in magnetosphere. The combination of the long period of these pulsations, their extended duration, the latitude-independent frequency, and the small azimuthal wave number suggests the occurrence of a global magnetospheric waveguide mode. The amplitude and cross-phase analysis of the wave activity on the ground and the polarization pattern indicate that the waveguide mode coupled to the field line resonance (FLR) occurs at different latitudes at different local times. Such FLRs occurred at latitudes smaller than usually observed at the same frequency, suggesting a significant reduction of the local field line eigenfrequencies as compared with usual values. A model estimation of such eigenfrequencies suggests a change in the magnetospheric field geometry characterized by more stretched field lines than those for usual conditions probably caused by the compression of the magnetosphere driven by the TD coupled with the stable northward orientation of the interplanetary magnetic field.
The appearance of type II radio bursts is mostly associated with flares and coronal mass ejections and other transient features. Propagating shock waves to the interplanetary medium can also be the cause to have a variety of radio emissions simultaneously. We analyzed well-separated (isolated) Decameter-Hectometer (DH) type II bursts which appear in the dynamic spectra without any earlier radio signatures. We studied 26 isolated DH type II bursts observed in 1998-2016. One explanation for the isolation of the DH type II bursts and delay in their observation time could be the occurrence of the flare-CME launch on the far side of the Sun. It could cause the emission to be observed only when the source gets high enough in the solar atmosphere. We found that only 30% of the bursts originated from the far side of the Sun, but also that no bursts originated from the central region of the Sun. Our analysis suggests that for the majority of isolated DH type II bursts a CME bow shock is more probable than a shock near the CME flanks. For 12 events we had observations from different viewing angles, from the instruments onboard Wind and STEREO satellites. Only five of them showed delays in the radio emission onset. Our analysis shows that in three events occultation could have been the cause of the delay in the emission onset. We also suggest that isolated type II radio burst needs specific conditions to form and be visible in the dynamic spectrum.
The energy spectrum of impulsive solar energetic electron events is believed to carry the imprint of the flare acceleration process which can be studied by analyzing the hard X-ray (HXR) spectrum of the flare. We have identified 17 energetic electron events well-observed with the SEPT instrument aboard STEREO which show a clear association with a hard X-ray (HXR) flare observed with the RHESSI spacecraft. We compare the spectral indices of the RHESSI HXR spectra with those of the interplanetary electrons. Because of the frequent double-power-law shape of the in-situ electron spectra, we pay special attention to the choice of the spectral index used for comparison.
We find a significant correlation of about 0.8 between the spectral indices of the HXR flare and the in-situ electrons. The correlations increase if only events with significant anisotropy are considered. This suggests that transport effects can alter the injected spectra leading to a strongly reduced imprint of the flare acceleration.
Although our results suggest a clear imprint of flare acceleration for the analyzed event sample, most of the studied events occur with onset delays at the spacecraft and in temporal coincidence with coronal mass ejections (CMEs). Therefore, a secondary acceleration, which would account for the observed onset delays, could be involved. However, the limited and variable pitch-angle coverage of SEPT could also be the reason for the observed delays.
The plasma dynamics at frequencies comparable with collisional frequency between various species has to be described in multifluid framework, where collisional interaction between particles is an important ingredient. In our study, we will assume that charged particles are strongly coupled, meaning that they form a single fluid that interacts with neutrals, therefore we will employ a two-fluid model. Here, we aim to investigate the evolutionary equation of slow sausage waves propagating in a gravitationally stratified flux tube in the two-fluid solar atmosphere in a strongly ionized limit using an initial value analysis. Due to the collisional interaction between massive particles (ions and neutrals), the governing equations are coupled. Solutions are sought in the strongly ionized limit and the density ratio between neutrals and charged particles is a small parameter. This limit is relevant to the upper part of the chromosphere. Our results show that slow sausage waves associated with charged particles propagate such that their possible frequency is affected by a cut-off due to the gravitational stratification. In contrast, for neutral acoustic waves the cut-off value applies on their wavelength and only small wavelength waves are able to propagate. Slow modes associated with neutrals are driven by the collisional coupling with ions.
Field aligned 1-D simulations of coronal loops show that density, temperature, and pressure do not vary much across the coronal loop. Consequently, such quantities averaged over the coronal part of the loop, can be used to characterize the loop's coronal part and its thermodynamic evolution. This is referred to as 0-D description of coronal loops, which provides an efficient method for conducting an approximate but quick study of the thermodynamic evolution of coronal loops. EBTEL2 is a commonly used 0-D code, which models the mass and energy exchange between the corona and the transition region. It solves for density, temperature, and pressure, averaged over the coronal part, velocity at the coronal base, and instantaneous differential emission measure distribution in the transition region. EBTEL2 assumes that the flows are subsonic at all stages, hence, neglects the kinetic energy term. However, in some cases, simulations using EBTEL2, show supersonic flows during the impulsive phase, while 1-D simulations by HYDRAD show subsonic speeds. This is a potential limitation to EBTEL2's usage. Therefore, it becomes important to have the solutions of the full energy equation. Here, we upgrade EBTEL2 by adding kinetic energy (referred to as EBTEL3). We compare the new solutions with those obtained using EBTEL2 and 1-D hydrodynamic code HYDRAD. EBTEL3 guarantees subsonic flows in cases where HYDRAD shows subsonic flows. However, when HYDRAD produces supersonic flows, EBTEL3 produces unreliable Mach numbers, and velocities, despite other quantities being reliable. A simple criterion for predicting situations where this happens, is also discussed.
The OI 135.56 nm line and CI 135.58 nm line are weak lines that are covered by NASA's Interface Region Imaging Spectrograph (IRIS) mission which studies how the solar atmosphere is energized. The emission in the OI 135.56 nm line is dominated by a recombination cascade. This line is optically thin and provides powerful diagnostics of unresolved velocity fields in the chromosphere. The CI line is optically thick and is dominated by a recombination cascade. Normally, the oxygen line is stronger than the carbon line but in flares, the ratio is opposite. The line intensities of oxygen and carbon peak at different times. The change in the ratio of CI/OI is due to an increase in the electron density in flares. We study the formation of the OI and CI lines in a 1D RADYN simulation of a flare to find out the cause of the change in ratio. For studying the line formation in a 1D atmosphere, we use the radiative transfer code RH to get a non-LTE solution with hydrogen, carbon and oxygen solved simultaneously.
Electric currents play a very important role in the energy balance of the solar atmosphere as they dissipate the energy stored in the magnetic field. In addition, electric currents can be used as proxies of non-potential magnetic fields, which are prone to produce enhanced chromospheric and coronal activity. Most previous measurements of electric currents have been limited to $j_z$. In this contribution we present a new method, based on the inversion of the radiative transfer equation for polarized light with magnetohydrostatic constraints (the Firtez-dz inversion code), that is able to reliably retrieve the three components of the electric current vector ${\bf j}$. In order to study to which accuracy we can determine electric currents we employ 3D MHD simulations to produce synthetic spectropolarimetric observations (i.e Stokes vector) via the forward solution of the radiative transfer equation. We then apply our newly developed inversion code to retrieve the electric currents from those synthetic observations and compare our inferences with the currents present in the MHD simulations. Our analysis shows that our method infers ${\bf j}$ within a factor or 2 of the original values in the solar photosphere.
Quiescent coronal cavities can provide insight into the solar magnetometry. They are observed in the coronal emission lines, both in polarized and unpolarized light. In the total linear polarization (L/I) they often possess a 'lagomorphic' structure that reflects the underlying magnetic field configuration. We performed analysis of 570 coronal cavities observed between 2012 and 2018 by the Coronal Multichannel Polarimeter (CoMP). The majority of cavities (82%) found in our study had a characteristic lagomorphic structure in linear polarization. We also compared cavity widths and sizes of the L/I signatures in order to evaluate the correlation between the two features. Our results suggest that observations of linear polarization in the solar corona are consistent with the theoretical model of cavity formation and structure.
It is critical to determine the solar disk's radiation in Mg II lines, e.g., to evaluate the radiation incident on solar chromospheric structures such as spicules or prominences, and to comprehend the radiation emitted by these structures in these lines. The aim of this project is to investigate the spatial and temporal variability of the Mg II h&k (2803.53 and 2796.35, respectively) lines in solar observations. Additionally, we seek to derive information on the spectral features of the Mg II h&k lines in the quiet sun at the centre of the sun. We present a novel approach for automatically determining the positions of k1v, k2v, k3, k2r, and k1r, as well as h1v, h2v, h3, h2r, and h1r, in the line profiles obtained by IRIS at the quiet sun centre. In this poster, we will address the variation in the spectral characteristics of the Mg II h&k lines in the quiet sun at the sun centre.
The solar chromosphere is critical in our understanding of the solar atmosphere energetics but poses important challenges both in observations and theoretical considerations. From an observational point of view, the number of spectral lines probing this layer are scarce and fall far apart (from UV to NIR). In this same direction, of special interest is the submilimiter continuum, whose different dependence with temperature as compared to the spectral lines, makes it an excellent observing asset. Thus, simultaneous observations of some of these regions typically involve the usage of disparate spatial resolutions.
In this contribution we present first results of a new inversion method applied to chromospheric analysis that consistently handles the effect of different spatial resolution and/or spatial sampling. This is done solving the inversion problem for the whole FOV at once and including in it the various spatial transformations and PSFs of each spectral range as linear transformations.
In this ISSI-supported series of studies on magnetic helicity in the Sun, we implement and systematically compare different magnetic helicity calculation methods on high-quality solar magnetogram observations. We apply finite-volume, discrete flux tube (in particular, connectivity-based), and flux-integration methods to magnetogram series from Hinode's Solar Optical Telescope. Finite-volume and connectivity-based methods yield instantaneous budgets of relative magnetic helicity (and free magnetic energy) in the active-region corona, while the helicity injection rate provided by the flux-integration methods yields an estimate of the accumulated helicity during the studied time interval. The observational target is the well-studied NOAA active region 10930 during a 1.5 day interval in December 2006 that included a major eruptive flare (SOL2006-12-13T02:14X3.4). The objectives of our work are twofold: a cross-validation of methods, as well as an interpretation of the complex events leading to the eruption. To the first objective, we find (i) strong agreement among the finite-volume methods, (ii) a moderate agreement between the connectivity-based and finite-volume methods, and (iii) an excellent agreement between the flux-integration methods. To the second objective, our analysis shows that the photospheric helicity flux significantly contributed to the coronal helicity budget, and that a previously emerged and/or formed right-handed structure (sheared arcade) erupted from a predominantly left-handed corona in the course of the X-class flare.
The Hydrogen Balmer lines show enhanced emission in various energetic phenomena in the solar atmosphere. For example, the H$\alpha$ line shows complex wing enhancements in the Ellerman Bomb phenomenon. Recently, Ellerman bombs have been detected in the H$\beta$ line at high number densities in the Quiet Sun and it was concluded that these mark the ubiquitous presence of small-scale magnetic reconnection. In this work, we explore the diagnostic potential of the H$\epsilon$ line, one of the shorter wavelength Balmer lines that promise detection of small-scale energetic events at higher spatial resolution than achieved before. H$\epsilon$ is located just redward of the strong Ca H line core which poses a challenge for the understanding of the spectral line formation. To understand the formation of H$\epsilon$, especially the transition from absorption to emission line, we investigate the line formation using 3D radiative MHD Bifrost simulations and NLTE forward modelling with RH. The locations where H$\epsilon$ goes into emission mark regions of steep chromospheric temperature enhancements and indicate regions where magnetic energy is released. H$\epsilon$ could be therefore a valuable tracer for small-scale energetic events in the solar atmosphere.
The magnetic helicity slowly and continuously accumulates in response to plasma flows tangential to the photosphere and magnetic flux emergence normal to it, it into the solar atmosphere. Analyzing the evolution of magnetic helicity flux at different atmospheric heights is key for identifying its role in the dynamics of ARs. The 3D magnetic field is obtained from PF extrapolations in order to derive the emergence, shearing and total magnetic helicity components at different atmospheric heights.
In this presentation, we show results obtained by analysing the evolution of the three magnetic helicity components in flaring and non-flaring ARs. The evolution of the three components reveals significant periodicities of them. In the flaring ARs, we found that the emergence, shearing and total helicity fluxes have common long periods as a function height in the solar atmosphere. In the case of non-flaring ARs, we do not find such common long oscillatory periods. This case study suggests that the presence of common significant long periodicities could help for a better understanding of the physics of the lower solar atmosphere, and, this oscillatory behaviour may even serve as a valuable precursor for flares.
We present the first results from the investigation of a filament eruption (FE) and associated ribbon flare, occurring in the southern solar hemisphere on 2021 May 9. Before the eruption, the filament was located in a plage region, close to the disk center and lay along the S-shaped magnetic polarity inversion line, i.e. it represented a sigmoid filament. The filament began to rise slowly at 09:30 UT and at 10:00 UT it erupted, which was accompanied by spreading ribbons at its base. During the FE, two flare ribbons slowly separated. During the ribbons evolution, hot post-flare loops (PFL) appeared at 11:00 UT and later, at 11:55 UT they formed PFL arcade.
Using the high resolution multi-wavelength data from the Atmospheric Imaging Assembly (AIA) onboard the Solar Dynamic Observatory (SDO) we study the kinematics and morphology evolution of the eruption and flare ribbons. The event was registered also by STEREO-Ahead Observatory, which allows us to explore the event kinematics and evolution from two different points of view.
The filament evolution before the eruption was traced by H-alpha data from the Global Oscillation Network Group. The photospheric magnetic field configuration was analyzed with the Helioseismic Magnetic Imager onboard the SDO.
Ubiquitous small-scale vortical motions that are generated on the solar surface at intergranular lanes by the turbulent dynamics of solar convection, are observed in the quiet-Sun atmosphere with dynamic timescales of a few minutes. Most of these convectively driven vortex motions harbour magnetic fields whose forced photospheric rotation often leads to the formation of magnetic tornadoes that penetrate several layers of the solar atmosphere and can reach heights up to the low corona. Both the formation of such magnetic structures and their uninhibited rotation strongly depends on the co-local magnetic field environment and topology, while the resulting twisting, braiding and dynamics of the magnetic field lines within them can drive and foster a wide variety of oscillations and wave modes. These modes include different Alfvenic type waves, such as kink, sausage, and torsional Alfven waves that could significantly contribute to the solar atmospheric heating at different heights. An analysis of recent high-temporal, high-resolution observations in the H$\alpha$ and Ca II IR lines, acquired with the Swedish Solar Telescope (SST), reveals more abundant small-scale vortical motions in the lower atmosphere than previously reported. We explore the role of the magnetic field in the formation of such vortical motions with the use of state-of-the-art magnetoconvection simulations. Moreover, exploiting both simulations and observations, we investigate the role of vortical structures in the small-scale dynamics of the quiet Sun, discuss the presence of Alfvenic type waves within them and provide estimates of the related energy transfer towards higher solar atmospheric layers.
Ellerman bombs are regions with enhanced Balmer line wing emission and mark magnetic reconnection in the deep solar atmosphere in active regions and quiet Sun. Recent observations suggest that Ellerman bombs are more prevalent than thought before. We aim to determine the occurrence of Ellerman bombs in the penumbra of sunspots. We analyze high spatial resolution observations of sunspots in the H-alpha and H-beta lines as well as auxiliary continuum channels obtained with the Swedish 1-m Solar Telescope. Features with all the defining characteristics of Ellerman bombs are found in large numbers over the entire penumbra. The true prevalence of these events is only fully appreciated in H-beta due to highest spatial resolution and lower chromospheric opacity. We find that the penumbra hosts some of the highest Ellerman bomb densities, only surpassed by the moat. Some penumbral Ellerman bombs show flame morphology and rapid dynamical evolution. Many penumbral Ellerman bombs are fast moving with typical speed of 3.7 km/s and sometimes more than 10 km/s. Many penumbral Ellerman bombs migrate from the inner to the outer penumbra over hundreds of km and some continue moving beyond the outer penumbral boundary into the moat. Many penumbral Ellerman bombs are found in the vicinity of regions with opposite magnetic polarity. We conclude that reconnection is a near continuous process in the low atmosphere of the penumbra of sunspots as manifest in the form of penumbral Ellerman bombs. These are so prevalent that they may be a major sink of sunspot magnetic energy.
Single fluid MHD theory is not able to fully describe observed plasma motions in solar prominences. Several authors (see Khomenko et al. (2016), Anan et al. (2017), Wiehr et al. (2019)) observed discrepancy between Doppler velocity measured in different spectral lines of ions and neutrals. However they give different answers to the question if motions of the plasma lead to decoupling of ions and neutrals as predicted by multi-fluid theory (see Popescu Braileanu et al.(2021)). In the current research we analysed observations of Doppler velocity in a quiescent solar prominence in 6 spectral lines of ions and neutrals acquired by HSFA-2 spectrograph in Ondrejov Observatory . We found discrepancy between measured Doppler velocity of ions and neutrals as well as between spectral lines of the same species. We found that apart from multi-fluid scenario effects of the radiative transfer should be included in interpretation.
In a recent work, Del Zanna et al. (2020, ApJ 898 72) have presented and discussed a new set of collisional-radiative models (CRMs) for helium in the quiescent solar corona, the largest of which includes fully LS-resolved set of states up to n=40 and n-resolved states up to n=300. Using those models, the corresponding emissivities for some important He I and He II lines relevant for DKIST, Solar Orbiter, and Proba-3 instruments have also been computed. We present here an extension of that work, which includes predicted line radiances of He II 30.4 nm, He I 1083.0 nm and 587.6 nm lines in various structures of the solar corona, and an analysis of the dependence of those radiances on various physical parameters such as electron density and temperature, photoexciting and photoionizing radiation fields.
Accurate understanding of the solar coronal temperature demands the study of Quiet Sun (QS) regions. In this work, we study quiet Sun data from 171 Å, 193 Å and 211 Å passbands of the Atmospheric Imaging Assembly (AIA) on board the Solar
Dynamics Observatory (SDO). We develop an uncertainty quantified machine learning inversion model to the empirical, statistical impulsive heating forward model of Pauluhn and Solank (2007) to infer the event frequency, timescale and the power law slope ($\alpha$) from the observations. On performing inversions across approx. 300,000 light curves per passband, we find that there are ≈ 2 − 3 impulsive events per min, with a lifetime of about 10 − 20 min. The $\alpha$ distribution is found to peak above 2 for all passbands. We then explore correlations among the frequency of impulsive events, their timescales and peak energy. The correlations suggest that conduction losses dominate over radiative cooling losses, and there might be a reservoir of energy either depleted by frequent, small events or infrequent, large events. All these findings suggest that impulsive heating is a viable heating mechanism in QS corona.
With the MPI-AMRVAC code, we present a 2.5-dimensional magnetohydrodynamic (MHD) simulation, which includes thermal convection and radiative cooling, to investigate the initial formation and long-term sustainment of coronal rain phenomenon. We perform the simulation in the initially linear force-free arcades which host a chromospheric, transition region, and coronal plasma, with turbulent heating localized on their footpoints after a relaxation to quiet solar atmosphere. Due to thermal instability, condensation starts at the loop top and becomes fragmented into smaller blobs. Following coronal rain dynamics for over 9 hours of physical time, we carry out a statistic study of the coronal rain blobs which quantify their widths, lengths, velocity distributions and other characteristics. We also track the movement of single blobs to study their dynamics and physical mechanisms behind them.
Solar prominences, the dense and cool materials embedded in the hot and tenuous corona, are intriguing structures in the solar atmosphere. To investigate the formation mechanisms of solar prominences, we reproduce two potential models, i.e., the levitation model and the reconnection and condensation model, by 2.5-dimensional magnetohydrodynamic (MHD) simulations in a chromosphere-transition-corona setup. In the levitation model, the initial arcade-like linear force-free magnetic field is driven by an imposed slow motion converging towards the magnetic inversion line at the bottom boundary. A magnetic flux rope (MFR) is formed by magnetic reconnection and eventually erupts as a coronal mass ejection (CME). An embedded prominence also gets formed directly by levitating material from the chromosphere. Synthetic images and light curves of the seven SDO/AIA channels and thermal X-ray are obtained with forward modeling analysis. In the reconnection and condensation model, a pre-existing MFR in the lower corona suddenly erupts due to catastrophe. The erupting MFR stretches the magnetic field lines, and a current sheet (CS) is formed. Multiple magnetic islands appear in the CS after plasmoid instability occurs. These magnetic islands carry mass from the chromosphere to the MFR. The dense and cool mass carried by the islands accumulated in the bottom of the MFR, forming a prominence. The condensation starts as the MFR rises. The coronal plasma continuously condenses into the prominence due to the thermal instability. We also study the dynamics and physical properties of the magnetic islands.
Recent observations by the Extreme Ultraviolet Imager (EUI) on board Solar Orbiter have revealed prevalent small-scale transient brightenings in the quiet solar corona termed "campfires". To understand the generation mechanism of these coronal brightenings, we constructed a self-consistent and time-dependent quiet-Sun model extending from the upper convection zone to the lower corona using a realistic three-dimensional radiation magnetohydrodynamic simulation. From the model we have synthesized the coronal emission in the EUI 174 passband. We identified several transient coronal brightenings similar to those in EUI observations. The size and lifetime of these coronal brightenings are mostly 0.5-4 Mm and ~2 min, respectively. These brightenings are generally located at a height of 2-4 Mm above the photosphere, and the local plasma is often heated above 1 MK. By examining the magnetic field structures before and after the occurrence of brightenings, we concluded that these coronal brightenings are generated by component magnetic reconnection between interacting bundles of magnetic field lines or neighboring field lines within highly twisted flux ropes. Occurring in the coronal part of the atmosphere, these events generally reveal no obvious signature of flux emergence or cancellation in photospheric magnetograms. These transient coronal brightenings may play an important role in heating of the local coronal plasma.
We study the various regions of the Sun, using high-resolution spectral observations from the Interface Region Imaging Spectrograph (IRIS). We observe the Quiet-Sun observation targeting the same region using different exposure times at different times and study the variation in the different parameters such as electron densities and filling factors using O IV line probing the transition region. We discuss the non-thermal width variations of Si IV line, as well. These observations will be able to provide better insights into interpreting upcoming new observations from Solar Orbiter SPICE spectrometer.
Metis is the coronagraph on-board Solar Orbiter, an ESA/NASA solar mission, launched in February 2020. At present, Solar Orbiter has completed the commissioning phase and it is in its cruise phase.
Metis is an externally occulted imaging coronagraph that provides imaging of the extended corona in ultraviolet and visible light. During these first phases, extensive observational campaigns have been carried out in order to characterize the response of the two Metis channels.
Amongst the different calibration and characterization activities already performed and planned for the future, an important role is played by stellar observations. Stars with known, stable fluxes are important to verify the radiometric response of the instrument over its field of view and monitor its evolution over time. Stars, being point-like sources, are also ideal to verify the spatial resolution of the instrument by gaining information on its point spread function (PSF).
In this work, we describe the first results obtained from the stellar calibration campaigns performed until April 2021.
We are studying MHD plasma turbulence generated by unidirectional surface Alfven waves, called ”Uniturbulence.” We analyze uniturbulence in the theoretical model with a sharp interface where surface Alfvén wave propagates. We consider an equilibrium configuration in a Cartesian coordinate system with a background magnetic field directed along the z-axis and no background flow. We take inhomogeneity perpendicular to the magnetic field. The surface Alfven waves that propagate along the field carry both Elsässer variables, Z$^\pm = $v$\pm $B$/\sqrt{\mu\,\rho}$. We calculate explicit expressions for the wave energy and energy cascade rate. We run the 3D ideal MHD simulations using the MPI-AMRVAC code. We demonstrate within a series of numerical simulations that the non-linear self-cascade of unidirectionally propagating waves obey the derived theoretical damping time scale equation:
\begin{equation}
\tau_d = \frac{6\,\sqrt{10}}{10\,V\,k_y}\frac{\zeta+1}{\zeta-1}
\end{equation}
$V$, $k_y$, and $\zeta$ are the velocity amplitude, wavenumber, and density contrast. This type of unidirectional cascade can play a role in heating the coronal plasma and driving the solar wind.
The recently discovered nanojets in a coronal loop (Antolin et al., 2021) were characterised in part by small (500-1500 km) and rapid (150-250 km/s) bursts of plasma ejected perpendicular to the field line of origin and accompanied by nanoflare-like intensity bursts in the UV and EUV. These nanojets were interpreted as a product of magnetic reconnection from small misalignments between the braided field lines, thus allowing to clearly identify the reconnection-driven nanoflare, and more generally, distinguish reconnection-driven coronal heating from wave-based coronal heating. The reconnection driver was found to be the partial loss of equilibrium of a nearby prominence but it was speculated that the nanojet should be largely independent from it. Furthermore, it is unclear how pervasive this phenomenon is. In this talk, we present new IRIS and SDO observations of nanojets found in multiple structures, namely in a solar blowout jet and in coronal rain loops. Their dynamics and morphology are in parallel with the previous findings. The reconnection events are further identified by the splitting of the field line origin. In multiple circumstances, we also observe that they occur in clusters, less than 1500km apart. While in the blowout jet case the Kelvin-Helmholtz instability is identified as the reconnection driver, the other 2 cases have a yet unclear origin. These observations in a variety of structures and environments suggest that nanojets are a general result of reconnection, and therefore, that they may play an important role in coronal heating.
The focus of many investigations on coronal wave heating has been on scrutinising the role of transverse (i.e. kink) modes; examining their damping by resonant absorption and the transfer of energy to Alfvén modes. Subsequently, the Alfvén modes are then subject to phase mixing and this leads to plasma heating. More recently, a non-linear mechanism for energy transfer has also been proposed, the so called uni-turbulence. Due to the ease with which they have been observed, the rapidly damped standing kink modes in active regions have spawned numerous studies investigating the role of resonant absorption in the observed damping. However, their counterparts in the quiet Sun, the propagating kink waves, have received little attention. Here I will discuss the results from a large-scale study of kink wave damping in the quiet Sun. We find convincing evidence that the damping of the kink waves is significantly weaker than in active regions and suggests that resonant absorption/phase mixing/uni-turbulence are not important for wave-based heating of the quiescent Sun. I will also discuss the physical reason we suspect is behind this result and what it tells us about the fine-scale structure of the quiescent corona.
We investigate the properties of plasmoids observed in the current sheet formed after an X-8.3 flare on September 10, 2017, using Extreme Ultraviolet (EUV) and white-light coronagraph images. The main aim is to understand the evolution of plasmoids at different Spatio-temporal scales using existing ground- and space-based instruments. We identified plasmoids in the current sheet observed in successive images of AIA and white-light coronagraphs, K-Cor, and LASCO/C2. We found that the current sheet is accompanied by several plasmoids moving upwards and downwards. Our analysis showed that downward and upward moving plasmoids have an average width of 5.92 Mm and 5.65 Mm, respectively in the AIA field of view (FOV). However, upward-moving plasmoids have an average width of 64 Mm in K-Cor which evolves to a mean width of 510 Mm in the LASCO/C2 FOV. Upon tracking plasmoids in successive images, we observe that downward and upward moving plasmoids have average speeds of ∼272 km/s and ∼191 km/s respectively in the EUV passbands. We note that the plasmoids become super-Alfvénic when they reach LASCO FOV. Furthermore, we estimate that the null-point of the current sheet at ~1.15 Rsun where bidirectional plasmoid motion is observed. We study the width distribution of plasmoids formed and notice that it is governed by a single power-law with an index of -1.12. Unlike previous studies, there is no difference in trend for small and large-scale plasmoids. The presence of accelerating plasmoids near the neutral point indicates a longer diffusion region as predicted by MHD models.
Developed in the framework of the H2020 SOLARNET project, the Solar Virtual Observatory (SVO) aims at making solar data more findable and accessible to the solar physics community. The SVO allows searching across multiple datasets as well as across the Heliophysics Event Database (HEK) and lets you search for data that overlaps with events from the HEK. It is conceived so that other event databases may also be linked to the SVO, such as for example for the ROB Event database that is soon to be publicly released. These capabilities will help researchers in discovering and accessing solar datasets from synoptic observations as well as solar data taken during short observation campaigns.
At the heart of the SVO lies a database populated with meta-data from datasets taken by space- and ground-based telescopes. It is designed to be easily interoperable with external tools and is accessible through a web interface as well as python and IDL clients.
Fundamentally different models are required for line emission in the corona compared to the chromosphere. Modelling the corona is remarkably straightforward by comparison, and the tendency for modellers and observers is to use coronal modelling in the transition region as well. Discrepancies with observations become obvious, however, when using the modelling for lines emitted by low charge ions.
To investigate more suitable modelling for the transition region, the coronal approximation is extended by including atomic processes which become more important further down in the atmosphere. These include the effects of higher density on free electron processes, and the influence of photo-ionisation and charge transfer. Models have been built for the main elements observed in this region (C, N, O, Ne, Mg, Si and S), and significant changes are seen compared to coronal modelling.
To assess how much the results reflect conditions in the transition region, line intensities are predicted using differential emission measure modelling. Observations of the quiet Sun show that a number of discrepancies are resolved for low charge ions when using the new modelling.
During solar flares, particles are accelerated to relativistic energies producing radio bursts at a large range of frequencies. The intensity of these radio bursts depends on their emission mechanism and the local conditions such as magnetic field strength, plasma density and the distribution of accelerated electrons. However, the presence of MHD waves in the loops can periodically change the local magnetic fields, resulting in modulations and oscillations of the observed radio bursts.
We examine microwave pulsations that occurred after a GOES C1.5-class flare and were observed with the Karl G. Jansky Very Large Array (VLA) at 1--2 GHz. VLA's high temporal resolution (50 ms), along with imaging spectroscopy, provides a detailed view of the pulsations. We also utilise the Solar Dynamics Observatory in extreme ultraviolet (EUV) and magnetic extrapolation to build a coherent picture. High brightness temperature (10^8 MK), polarisation properties accompanied by suitable magnetic field strengths, and coronal density suggest Electron-Cyclotron Emission (ECM). The microwave pulsations are observed from 1 GHz to 1.5 GHz exhibit 4.5 secs for all frequency channels, most likely caused by Sausage mode oscillations. The imaging shows multiple source locations non-cospatial with flare location. The magnetic extrapolation reveals the magnetic connectivity from the flare location to the microwave sources providing channels for the energetic particles from the flare site to the radio source location. I will discuss the detailed results and physical interpretation of the microwave pulsations seen for the event.
We have analysed solar activity using simultaneous observation of Solar Dynamics Observatory (SDO), Solar Terrestrial Relations Observatory (STEREO), Parker Solar Probe (PSP), and GOES missions. We studied the M4.4 class solar flare that occurred around 13:00 on 29th November 2020 in the active region (AR 12790) and the related CME. The flare is observed at the solar limb by the SDO and close to the disk center by STEREO. We analysed data from SDO-AIA, STEREO-EUVI to determine the potential source of the type II and III radio bursts observed by PSP. To this aim, we studied the flare brightness and topology evolutions and the CME velocity propagation. Using the PSP-RFS data and a model of the heliospheric density, we estimated the electron density, the height where the type II and III bursts are created and, electron velocity related to these bursts. The new PSP data allows us to investigate the radio-emission unprecedently close to the Sun with improved sensitivity. Moreover, we analysed the EIT (EUV) wave observed by STEREO-SECCHI, producing a widespread of solar energetic particles in the heliosphere. Based on the above measurements, we built the comprehensive image of the solar eruption. First, the SDO&STEREO observations showed a flare and associated EIT wave. The type III radio-burst is associated with electrons beams that are accelerated by magnetic field reconnection during the flare. Then, the CME is propagated. The type II radio-burst is related to propagation of a MHD wave in the corona resulting from CME propagation.
We summarize our science preparations for the Lyman-alpha Solar Telescope (LST) aboard the Chinese ASO-S mission. LST has the capability to simultaneously observe the Sun from the solar disk to 2.5 solar radii in both Lyman-alpha and visible light. Our particular interests are CMEs, flares, and prominences in the new Lyman-alpha waveband. We Synthesize these eruptive features in Lyman-alpha based on various numerical simulations concerning both optically thin and thick regimes. Their statistical and case studies based on Lyman-alpha measurements from GOES/EUVS, SOHO/UVCS and so on are also included to reveal flare and CME properties and develop physical diagnostic tools. The synergy with Solar Orbiter/Metis and EUI are discussed as well.
The Extreme Ultraviolet Imager (EUI) onboard Solar Orbiter (SolO) observed an eruption with its Full Sun Imager (FSI) in both of its channels (17.4/30.4 nm), on 2021-April-22. At the time, the spacecraft was at 0.87 au from the Sun. The eruption was seen at the SW limb, starting at 04:24 UT, with the source slightly backside as seen from SolO (S20W103). From the Earth’s perspective, SDO/AIA and PROBA2/SWAP observed a wave and dimmings starting around 04:07 UT, on-disk at ~S20W05. STEREO-A/EUVI saw similar signatures of an eruption starting around 04:17 UT, on-disk at ~S20W50.
The corresponding CME was visible shortly after in several coronagraphs. SOHO/LASCO-C2 observed a full halo CME starting around 06:00 UT. STEREO-A/COR2 recorded a clear structured CME seen from around 05:23 UT. SolO Metis data will be analysed as it becomes available.
SolO/STIX observed the associated X-ray flare, which was partially occulted. This allows the characterization of both the thermal plasma and any potential contribution of nonthermal electrons in the tenuous coronal source. The X-ray source location will be compared to the EUV coronal structures. The full-Sun radiometer PROBA2/LYRA also observed the event with the two SXR channels.
The corresponding ICME arrived at the Earth on 2021-April-24-25 (probably also at STEREO-A), it was driving a shock and created minor geomagnetic storm conditions. STEREO-A/SEPT and ACE/EPAM observed a weak particle event most likely related to this eruption. We will analyse in depth these CME-ICME connections.
In my talk I will present a statistical study of flares on solar-type stars based on TESS (Transiting Exoplanet Survey Satellite) observations. We used a two-minute cadence data obtained from sectors 1 - 36. Our software allows us to identify flares and determine its parameters such as: amplitude, duration, growth and decay times. Furthermore, we estimate the maximum luminosity and total energy of flares in two different methods. In the first two years of TESS observations, we already identified about 14000 flares from more than 4000 solar-type flaring stars. Based on bolometric flare energy distribution, we conclude that its energies range from 10^32 to 10^37 erg, with an average energy of 10^34 erg. Our study suggests that there are two types of flare events, described by different profiles.
The launch of the Solar Dynamics Observatory (SDO) with the Helioseismic and Magnetic
Imager (HMI) and the Atmospheric Imaging Assembly (AIA) instruments, is the first time that both a vector magnetograph and ribbon-imaging capabilities became available on the same observing platform. This combination presented a first chance to do statistical studies of the properties of the vector magnetic fields participating in the flare. Here we present a statistical analysis of spatial and temporal properties of the vector magnetic fields in 40 active regions associated with flares, of GOES class C9.0 and greater. For every event in the database, we use 1) a pre-flare vector magnetogram from HMI/SDO, to describe magnetic field properties before the flare and 2) a sequence of AIA 1600A images, to track location of flare ribbons. We calculate the following physical properties of the photospheric vector magnetic field within the active region, flare ribbons and the polarity inversion line: magnetic flux, magnetic shear, vertical electric current and current neutralization. We present the results and discuss their meaning in the context of the standard flare model.
Quasi-periodic pulsations (QPPs) refer to nearly-periodic oscillations that are often observed in irradiance time series during solar flares and have also been reported in several stellar flares. In the last years, several statistical studies based on Soft X-ray measurements have reached the conclusion that QPPs are present in most solar flares of class M and above.
However, QPPs sometimes exhibit different properties. In particular, QPPs with periods of the order of 20s have been detected during the impulsive phase of most flares, but longer periods are also sometimes present and tend to persist in the decaying phase of flares. Also, for some events, the period has been reported to increase as the flare evolves, which has been correlated with the evolution of the ribbon separation. But again, this behavior does not seem to happen systematically.
All this could point to the coexistence of QPPs with different origin mechanism.
Recently, QPPs were also detected in the Lyman-alpha observations of solar flares. As most of the Lyman-alpha flare emission is likely produced at the footpoints of the flaring loops, when the beam of electrons accelerated during the magnetic reconnection at the origin of the flare reaches the chromosphere, the Lyman-alpha observations are expected to behave similarly to non-thermal emission, contrarily to SXR observations.
In this poster, we compare the characteristics of QPPs detected in Lyman-alpha observations by PROBA2/LYRA, GOES‐15/EUVS‐E, etc., to those in the SXR with the aim of getting additional information to help differentiating between the mechanisms at their origin.
Powerful solar phenomena, such as flares, coronal mass ejections, affect the space environment, the dynamics of near-Earth space. As a rule, sudden disturbances in the near-earth space environment can cause disruptions in the operation of various communication systems, of ground-based electrical energy systems. In this regard, it is relevant to develop recommendations for identifying geoeffective solar phenomena that cause unfavorable magnetic ionospheric disturbances. The use of solar radio emission for solving the problems posed seems to be effective due to the fact that practically all processes occurring on the surface of the Sun and its atmosphere are reflected in radio emission. The report presents the main results of studies on the development of methods for determining the degree of geoeffectiveness of powerful and proton solar flares, coronal mass ejections from solar radio emission data.
The work was carried out under the project No. 0729-2020-0057 within the framework of the basic part of the State assignment of the Ministry of Science and Higher Education of the Russian Federation.
The results of studies the influence of solar phenomena, such as coronal mass ejections (CMEs) and high-speed solar wind streams (HSS), on the characteristics of the ionosphere are presented. A set of space weather parameters (type and speed of coronal mass ejections, X-ray flux, high-speed solar wind velocity) is considered, which made it possible to reveal the dominant physical connections between the dynamics of the ionosphere and these two solar phenomena. The study uses data from vertical and oblique sounding of the ionosphere obtained during several solar events that occurred in the 24 solar cycle. It is shown that CME and HSS are global events of solar activity that affect the parameters used to characterize the ionosphere.
The work was carried out under the project No. 0729-2020-0057 within the framework of the basic part of the State assignment of the Ministry of Science and Higher Education of the Russian Federation.
One of the main goals of solar physics is the timely identification of eruptive active regions. Space missions such as Solar Orbiter or future Space Weather forecasting missions would largely benefit from the achievement of this goal. Our aim is to show how a physics based technique can provide real time indications that an active region will produce an eruption with a simple green/amber/red risk of eruption. We expand on work of Pagano et al., 2019a,b that was able to define a theoretical and operative metrics that discriminate eruptive from non-eruptive active regions by analysing the Lorentz force in a 3D dynamic reconstruction of the magnetic field configuration of active regions with magnetofrictional simulations. In this work, we finalise the metric to include the effects of magnetic flux emergence and solar flares. We therefore obtain the operative framework of the StAndrews Space Weather Active Region Monitoring (S2WARM) and we show how this can be used by space weather forecasters to derive useful information on active regions in the Sun. To do so, we apply the S2WARM technique to a time period of 45 days in 2013 when several active regions crossed the solar disk, as we individually model their magnetic field configuration evolution and benchmark S2WARM metric against observational signature of flux rope ejections and flares. We find that our technique provides correct identifications of eruptive or non-eruptive active regions in 82% of the cases and we also illustrate how to apply this technique in various space weather forecasting applications.
We study the evolution of stream and co-rotating interaction regions (SIRs and CIRs) as they propagate from Earth to Mars. We incorporate solar wind plasma and magnetic field data from the OMNI database and the Mars Atmosphere and Volatile EvolutioN (MAVEN) spacecraft. Additionally, we use images from the Solar Dynamics Observatory (SDO). The investigation covers the declining phase of solar cycle 24, resulting in a clean dataset of 146 events at 1 AU and 126 events at 1.5 AU. We perform a superposed epoch analysis (SEA) of bulk speed, number density and temperature, as well as magnetic field magnitude and total perpendicular pressure. We conduct an in-depth analysis for a subset of events during the opposition phases of the two planets. In-situ properties of SIRs are linked to the extension of their source coronal holes (CHs) for this period of time. The SEA reveals a broadening of SIRs at the wave crest by 17% for speed, and by about 45% for both magnetic field magnitude and total perpendicular pressure. The amplitudes of the normalized solar wind parameters increase monotonically from Earth to Mars, except for that of plasma temperature, which shows a decrease. We arrive at similar correlations for streams at both planets during the opposition phases. There is a stronger linkage of maximum solar wind speed to the latitudinal extension of CHs than to their longitudinal extent. We find that the occurrence rate of fast forward shocks increases by a factor of three from Earth to Mars.
An important aspect in the early evolution of a coronal mass ejection (CME) is its interaction with the magnetic field in the low corona on its way to the heliosphere. This interaction can influence the trajectory and morphology of the eruption, so a better understanding of this field/eruption coupling could lead to better constraints on the inputs into Space Weather forecasting models. Here we report on a simulation of a CME with a complex evolution in the low corona. The CME originates from the eruption of a filament channel formed beneath a pseudostreamer. The eruption interacts with both the pseudostreamer and an adjacent helmet streamer producing a coupled eruption involving both structures. As a result, the CME produced is strongly deflected and contains a mixture of open and closed magnetic flux. Our simulation covers the full length of the eruption process, from formation of the filament channel to propagation of the CME out to 30 solar radii, allowing an in-depth look at the how the CME forms and evolves. This work demonstrates the importance of the global coronal magnetic field in the formation process of some CMEs.
The Doppler velocities observed in the solar photosphere are known to show significant center-to-limb variation. The convective blueshifts observed near the disk center decrease toward the limb and they turn into redshifts, which is called the limb effect. This is produced by the projection of the 3D atmospheric structure along the line of sight. The previous studies using ground-based telescopes and numerical simulations were done from 0 to 80 degrees in the heliocentric angle. To study the limb effect very close to the limb, we analyzed the Doppler velocities of the Fe I 630.15 nm line using Hinode SOT/SP data. The high spatial resolution of the SOT enables us not only to resolve the photospheric structure but also to see the line as an emission profile just above the limb. The data shows decreases in the blueshift toward the limb and almost constant above 80 degrees. Classifying the spectra into those from granules, intergranular lanes, and magnetic regions, we found the granules show the center-to-limb variation, but the intergranular lanes do not show it. The bisector analysis of the line profiles in the granules show the largest velocity difference between line core and near wing of 300 m/s at around 75 degrees. The emissions of the Fe I line above the limb are clearly blueshifted compared to the absorptions within the solar disk near the limb. The 3D structures of the solar surface could be inferred from this analysis of the Doppler velocities near the solar limb.
The Metis coronagraph, on board the Solar Orbiter (SolO) mission, records full-Sun images of the solar corona in ultraviolet and in polarized visible brightness (pB). The range of heliocentric heights covered by the field of view (FoV) of Metis changes as a function of the SolO position along its highly eccentric orbit. For its maximum aphelion distance ($\approx 1~\text{au}$) the radial FoV of Metis is $\approx 5.8-10.2~\text{R}_\odot$, while for its minimum perihelion distance ($\approx 0.3~\text{au}$) it is $\approx 1.7-3.1~\text{R}_\odot$. Also, as the angular velocity of SolO around the Sun changes along its orbit, so it does the time required to observe the Sun from different view angles. In this work, we explore the use of Metis pB images for tomographic reconstruction of the three-dimensional (3D) distribution of the coronal electron density. Using the predictive orbital information of SolO and the specifications of the Metis instrument, we compute synthetic images of the solar corona based on a 3D MHD steady state coronal model. We use these images as data for tomographic reconstructions. We carry out these simulations for an aphelion and a perihelion location. We conclude that a $\sim 4$ image/day synoptic program will provide enough images to carry out tomography with Metis images at any point of the SolO orbit. We discuss in detail what region of the solar corona can be reconstructed as a function of the orbital location.
Using Atacama Large Millimeter/submillimeter Array (ALMA) observations of the quiet Sun at 1.26 and 3 mm, we study spatially resolved oscillations and transient brightenings, i.e. small, weak events of energy release. Both phenomena may have a bearing on the heating of the chromosphere. At 1.26 mm, in addition to power spectra of the original data, we degraded the images to the spatial resolution of the 3 mm images and used fields of view of equal area for both data sets. The detection of transient brightenings was made after the oscillations were removed. At both frequencies we detected p-mode oscillations in the range 3.6-4.4 mHz. In the corrected data sets, the oscillations at 1.26 and 3 mm showed brightness temperature fluctuations of ~1.7-1.8% with respect to the average quiet Sun, corresponding to 137 and 107 K, respectively. They represented a fraction of 0.55-0.68 of the full power spectrum and their energy density at 1.26 mm was 0.03 erg/cm$^3$. We detected 77 transient brightenings at 1.26 mm and 115 at 3 mm. Although the majority of the 1.26 mm events occurred in cell interior, their occurrence rate per unit area was higher than that of the 3 mm events. The computed low-end energy of the 1.26 mm transient brightenings ($1.8 \times 10^{23}$ erg) is among the smallest ever reported, irrespective of the wavelength of observation. However, their power per unit area is smaller than that of the 3 mm events, probably due to the detection of many weak 1.26 mm events.
Fan-shaped jets can be observed above light bridges and are driven by reconnection of the vertical umbral field with the more horizontal field above the light bridges. Because these jets are not fully opaque in chromospheric lines, one cannot study their spectra without the highly complex considerations of radiative transfer in spectral lines from the atmosphere behind the fan.
We take advantage of a unique set of critically sampled polarimetric observations of the Halpha, CaII 8542Å and CaII K lines obtained with the Swedish 1-m Solar Telescope to study the physical properties of a fan-shaped jet that was backlit by an X9.3 flare. The Halpha flare ribbon emission profiles from behind the fan are highly broadened and flattened, allowing us to investigate the fan with a single slab via Beckers' cloud model (Beckers 1964), as if it were backlit principally by continuous emission. From this we derived the opacity and velocity of material in the jet.
For the first time, we report estimates of the mass and density in a fan-shaped jet. Using inversions of CaII 8542Å emission via STiC (STockholm inversion Code; de la Cruz Rodríguez+ 2016; de la Cruz Rodríguez+ 2019), we were also able to estimate temperature and cross-check the velocity of material in the jet.
Finally, we use the masses, plane-of-sky and line-of-sight velocities as functions of time to investigate the supply of momentum to the photosphere in the collapse of this jet, and evaluate it as a potential driver for a Sunquake beneath.
Heat fluxes from Type II spicules into the surrounding corona as a possible source of corona heating are determined. We have shown that in order to compensate for radiation and thermal conduction losses, approximately 10^4 hot Type-II spicules are required, which is about 1% of the number of spicules simultaneously observed on the solar disk. The main driver for coronal heating is the convective motion of the photosphere which creates emf. The emf supports the electric current in the Type II spicule and the dissipation of the current in the partially ionized plasma heats the spicule to the temperature > 1 MK. Arguments in favor of Type-II spicule as an open magnetic flux tube are given. The analysis shows also that Type-II spicules play an important role in the replenishing the solar corona with hot plasma.
By V.V. Zaitsev and A.V.Stepanov
Light bridges (LBs) are elongated and bright structures that seem to be related to the formation and evolution of sunspots. In this contribution, we present the results of long-term evolution of different atmospheric parameters of three LBs formed in the same host sunspot by different mechanisms. We have used data taken with the GREGOR Infrared Spectrograph installed at the GREGOR telescope. These data were inverted to infer the physical parameters of the atmosphere where the observed spectral profiles were formed. In particular we focus on the magnetic field strength, inclination, and temperature values of the LB as well as its comparison to the surrounding umbra and penumbra. We found that the general behaviour of the three LBs is typical of this kind of structures with the magnetic field strength, inclination, and temperature values between the values at the umbra and the penumbra. In addition, each LB show particular behaviours that are likely related to the different nature of each LB.
Energy transport through thermal conductivity is an important mechanism in the solar corona. Here we report on the implementation of thermal conductivity into the MANCHA code, which allows its extension to corona. Conductivity is frequently modeled with the expression deduced by Spitzer in the limit of the strong magnetic field which restricts the effects to the corona. However, for an accurate description of the complete solar atmosphere, the thermal conductivity should be modeled through all the layers. We present a numerical study of thermal conductivity effects from the photosphere to the corona. We use the model developed by Braginkii for the electron heat flux for a magnetic field with an arbitrary strength. For completeness, we carry on simulations using the limits of strong magnetic field and weak magnetic field as well. Super-time-stepping scheme is applied to deal with the limitations on the integration time step imposed by the conductivity. The validation of the thermal conductivity implementation is carried out with standard tests in one, two, and three dimensions.
Spatially unresolved data shows that the cooling phase in solar flares can be much longer than theoretical models predict. It was not yet determined whether this is also the case for different sub-regions within the flare structure.
Two questions are in the focus of this case study: 1. Are the cooling times, which are observed separately in coronal loops and the supra-arcade fan (SAF), in accordance with the existing cooling models? 2. Do the supra-arcade downflows (SADs) have different temperature and emission measure than their surrounding? An M5.6 limb flare on 13 January 2015 is analysed by using SDO/AIA data. A differential emission measure (DEM) reconstruction code derives spatially resolved temperature and emission measure maps. This output is used to investigate the thermal evolution of coronal loops, the supra-arcade fan (SAF), and the supra-arcade downflows (SADs).
Observational evidence shows that coronal jets can hit prominences and set them in motion. The impact leads to large-amplitude oscillations (LAOs) in the prominence. We attempt to understand this process via 2.5D MHD numerical experiments. The jets are generated in a sheared magnetic arcade above a parasitic bipolar region located in one of the footpoints of the filament channel (FC) supporting the prominence. The shear is imposed at velocities not far above the observed photospheric values; this leads to a multiple reconnection process, as obtained in previous jet models. Both a fast Alfvénic perturbation and a slower supersonic front preceding a plasma jet are issued from the reconnection site; in the later phase, a more violent (eruptive) jet is produced. The perturbation and jets run along the FC; they are partially reflected at the prominence, and partially transmitted through it. This results in a pattern of counter-streaming flows along the FC, and oscillations in the prominence. The oscillations are LAOs (i.e., with amplitudes above 10 km s−1) in some areas of the prominence, both in the longitudinal and transverse directions. In some field lines, the impact is so strong that the prominence mass is brought out of the dip and down to the chromosphere along the FC. Two cases are studied, with respect to arcades at different heights above the parasitic bipolar region, leading to different heights for the region of the prominence perturbed by the jets. The oscillation amplitudes and periods are in general agreement with the observations.
The Metis coronagraph is one of the remote sensing instruments of the Solar Orbiter mission launched on February 10, 2020. Metis is an innovative externally occulted coronagraph designed to observe the solar corona in an annular field of view from 1.6deg to 3deg simultaneously for the first time in the broadband linearly polarised visible light and in the narrow-band HI 121.6 nm (Lyα).
Metis has been characterised during the three-month long commissioning phase and throughout the cruise phase that will end after the Earth fly-by on November 27, 2021, official start of the nominal mission phase.
In this work the Metis performance and main scientific achievements will be reviewed.
Coronal streamers are long lived structures of the solar corona, and are very important source of slow solar wind. We have analyzed few dozen of coronal streamers observed by AIA/SDO, from solar activity maximum to minimum. For each streamers we applied a Differential Emission Measure method to obtain both a temperature distribution and a value of average temperature as well as it’s change with height above photosphere. We find that streamers are filled with plasma with temperatures in the range of 1.2-2.0 MK. We found that average temperatures of streamers changes as a function of solar activity phase.
In this work we use realistic three-dimensional (3D) radiative-MHD simulations of the chromosphere to model distribution of radio brightness over the solar disk and radio radius at millimeter wavelengths. We compare modeled center-to-limb variations with the observed behavior derived from diverse historical measurements as well as from recent observations. Our results show that the model distribution of millimeter brightness resembles the observed dependencies up to the distance of 0.95R. We report the model value of the radio radius (excess over the optical radius) to be in the range of 3-4 arcsec for the entire millimeter range, which is significantly smaller than the observed values (5-12 arcsec). The possible reasons of the found discrepancy between the models and observations in the near-limb zone are discussed.
High-resolution spectropolarimetric ground-based observations, complemented with data from the space instruments, allow us to investigate the photospheric magnetic and velocity properties of sunspot penumbra during the formation and decay phases. The observed penumbral formation occurs only on one side of the studied region. This preferential location appears to be due to the absence of an overlying magnetic canopy, as derived from potential field extrapolations of the SDO/HMI data. Then, the studied penumbra disappears progressively in both time and space. The progressive disappearance of different penumbral sectors seems to be linked with the presence or absence of overlying canopies. Noticeably, we detect Evershed flows and horizontal fields after the apparent disappearance of the penumbral sectors.
The propagation of Alfven waves with periods > 10 s in the stratified isothermal atmosphere has been considered. Based on the numerical simulation the dependence of the wave energy flux on the height at different values of wave periods has been calculated. It has been shown that the so-called tuning points («cutoff frequencies») could not be used for the description of wave energy flux. The results are interpreted on the basis of the oscillation theorems and phase relationships between perturbed velocity and magnetic field. The process of continuous reflection of Alfven waves in the solar atmosphere is discussed.
This work was supported in part by the Russian Foundation for Basic Research (project no. 20-52-26006) and the Ministry of Education and Science (NIR no. 0831-2019-0006).
The equilibrium of the axisymmetric cylindrical magnetic flux rope under solar coronal conditions in the light of the paradigms of Severny and Parker connected with the existence of neutralized and non-neutralized electric currents in the solar photosphere is considered. Based on the generalized Gold-Hoyle force-free magnetic field configuration it has been shown that only the non-shielded (non-neutralized) flux ropes can provide the sufficiently strong (> 100 G) magnetic field concentration at quite small (< 10) values of the number of turnsof magnetic field lines over the loop length. The formation of corona flux ropes and their MHD stability are discussed.
This work was supported in part by the Russian Foundation for Basic Research (project no. 20-52-26006) and the Ministry of Education and Science (NIR no. 0831-2019-0006).
Using data from the Helioseismic and Magnetic Imager on board the Solar Dynamics Observatory (HMI/SDO) on the magnetic field vector in the solar photosphere, we analyzed the structure of magnetic fields and vertical electric currents in six active regions (ARs) with different levels of flare activity. Decomposition of the transverse magnetic field vector into two components allowed us to reveal the existence of vortex structures of the azimuthal magnetic field component covering a large area around the main sunspots of an AR, which indicates to a presence of the distributed over large area electric current system. The low value of the vertical electric current imbalance over the entire AR (below 0.1%) suggests that the distributed electric current is closed within an AR. We calculated the distributed electric currents in all analyzed ARs and studied their temporal variations and the relationship with the flare productivity of an AR. It was found that low-flaring ARs exhibit small variations of the distributed current in the range of ±20×10^12 A, whereas the highly flaring ARs exhibited significant smooth variations of the distributed current in the range of (30-95)×10^12 A. Intervals of the enhanced flaring appear to be co-temporal with smooth enhancements of the distributed electric current.
Coronal loops are building blocks of solar active regions. However, their formation mechanism is still not well understood. Here we present direct observational evidence for the formation of coronal loops through magnetic reconnection as new magnetic fluxes emerge into the solar atmosphere. Extreme-ultraviolet observations of the Atmospheric Imaging Assembly (AIA) onboard the Solar Dynamics Observatory (SDO) clearly show the newly formed loops following magnetic reconnection within a plasma sheet. Formation of the loops is also seen in the Hα line-core images taken by the New Vacuum Solar Telescope. Observations from the Helioseismic and Magnetic Imager onboard SDO show that a positive-polarity flux concentration moves towards a negative-polarity one with a speed of ~0.4 km/s before the formation of coronal loops. During the loop formation process, we found signatures of flux cancellation and subsequent enhancement of the transverse field between the two polarities. The three-dimensional magnetic field structure reconstructed through a magnetohydrostatic model shows field lines consistent with the loops in AIA images. Numerous bright blobs with an average width of 1.37 Mm appear intermittently in the plasma sheet and move upward with a projected velocity of ∼114 km/s. The temperature, emission measure and density of these blobs are about 3 MK, 2.0×10^28 cm^−5 and 1.2×10^10 cm^−3, respectively. A power spectral analysis of these blobs indicates that the observed reconnection is likely not dominated by a turbulent process. We have also identified flows with a velocity of 20 to 50 km/s towards the footpoints of the newly formed coronal loops.
Structures and heating mechanism of microflares have been unclear, but which is promising to be resolved with coming Solar Orbiter data combined with other ground-based telescopes of ultrahigh temporal and spatial resolution observations. Here, we analyze 3D magnetic structures and heating mechanism of a microflare based on three-dimensional radiative magnetohydrodynamic simulation of a solar quiet region. The simulation is conducted with MURaM code in a box including the upper convection zone, the photosphere, the chromosphere, and the low corona. We find that the microflare is produced above the polarity inversion line between a small negative polarity and a dominant positive polarity. The locations of the strongest EUV emissions are identified to be cospatial with that of the fast energy release rate. With a magnetic topology analysis, a 3D fan-spine magnetic topology is found to be a possible reason to allow the energy release. Moreover, the microflare is also companied with obvious flux cancellation, however, which is found not to play an important role to cause this confined flare.
The triggering process for prominence instability and consequent CMEs is not fully understood. Prominences are maintained by the Lorentz force against the gravity, therefore reduction of the prominence mass due to the coronal rain may cause the change of the force balance and hence destabilization of the structures.
We aim to study the observational evidence of the influence of coronal rain on the stability of prominence and subsequent eruption of CMEs.
We used the simultaneous observations from AIA/SDO and SECCHI/STEREO spacecrafts from different angles to follow the dynamics of prominence/filaments and to study the role of coronal rain in their destabilization.
Three different prominences/filaments observed during the years 2011-2012 were analyzed using observations acquired by SDO and STEREO. In all three cases, massive coronal rain from the prominence body led to the destabilization of prominence and subsequently to the eruption of CMEs. The coronal rain triggered the initial slow rise of prominences, which led to the final instability (probably by magnetic reconnection) after 18-28 hours in all cases. The estimated mass flux carried by coronal rain blobs showed that the prominences became unstable after 40 % of mass loss.
We suggest that the initial slow rise and the consequent instability of prominences could be connected with their mass loss by massive coronal rain and breakout model, respectively. If this is the case, then the coronal rain can be used to predict the CMEs and hence to improve the space weather predictions.
High-resolution solar observations show the complex structure of the magnetohydrodynamic (MHD) wave motion. We apply the Proper Orthogonal Decomposition (POD) and Dynamic Mode Decomposition (DMD) techniques to identify the dominant MHD wave modes in a sunspot with a circular cross-sectional shape, using the intensity time series. The POD technique was used to find modes that are spatially orthogonal, whereas the DMD technique identifies temporal orthogonality. Here we show that the combined POD and DMD approaches can successfully show the appearance of both the slow body sausage and kink modes in a sunspot umbra with an approximately circular cross-sectional shape.
One of the possible reasons for heating both open and closed magnetic field regions of the solar corona is due to the MHD turbulence. In this work, we have estimated the density filling factor which plays a crucial role as a correction factor for the energy flux for the Alfv{\'e}n waves and kink waves. We have employed an ideal 3D MHD simulation for an open magnetic structure using MPI-AMRVAC by incorporating density inhomogeneities in a background atmosphere along the transverse direction of the magnetic field for a spatial domain of 50 Mm $\times$ 5 Mm $\times$ 5 Mm. Once the simulation reaches equilibrium, we excite the system by implementing transverse MHD waves at the base of the simulation domain. The presence of the transverse inhomogeneities leads to the generation of turbulence, which creates density irregularities (or structure irregularities) in the atmosphere. We estimate the filling factor by two different methods: (i) by calculating the fraction of the volume which is more than a density threshold to the entire volume of the simulation domain, and (ii) from the synthetic observations of the LOS intensity from the line ratio of the Fe XIII 10749\AA \ and 10800\AA \ density sensitive line pairs by the spectroscopic forward modeling using FoMo. The results obtained from both methods are in reasonable agreement with the observations of coronal holes, coronal loops, and fan-like structures. We also infer from the obtained results that the generation of turbulence increases the density filling factor of the medium.
Oscillations in solar active regions are mainly due to leakage of
acoustic oscillations that are trapped inside the Sun. Doppler
velocity and intensity measurements are known to clearly show these
oscillations in magnetic structures. In recent years, magnetic field
fluctuations have been reported in both the photosphere and
chromosphere. The reason for these observed oscillations in the
magnetic field has been difficult to interpret. In this work, to
address this issue, we invert temporal series of sunspot observations
in the He I 1083 nm line using HAZEL. The nature and origin of
these magnetic field fluctuations are interpreted with the support of
numerical simulations.
Three-dimensional (3D) magnetohydrodynamic simulation is performed to explore the process of magnetic reconnection at the 3D magnetic nulls and quasi-separatrix layers (QSLs). The initial magnetic field is constructed analytically by superposing uniform vertical magnetic field on a linear force-free field. The initial field is characterized by the presence of a pair of 3D nulls along with quasi-separatrix layers. The topology of the 3D null, complete with the spine-axis and the dome-shaped separatrix surface, is similar to the ones expected in the solar corona. The simulated evolution documents the movement of the field lines of the separatrix surface to be different than the field lines located in the vicinity of the surface. This generates favorable contortion in the field lines to develop current sheets, which are localized to the separatrix surface --- giving rise to the torsional fan magnetic reconnections at the 3D nulls. Additionally, the reconnections are also found to occur at the QSLs. However, the strength of the currents near QSLs is smaller than the strength at the fan surfaces of the 3D nulls, which indicates the reconnections near QSLs to be less energetically efficient than the 3D nulls.
Solar flares are an explosive manifestation of complex magnetic loop reconfigurations in the vicinity of active regions in the solar atmosphere. During a flaring event, the magnetic field topology changes rapidly, abruptly, and significantly. Some of these eruptive events inject enough energy into the photosphere and sub-photosphere to generate acoustic responses observed as sunquakes. The precise physical mechanism causing the acoustic source of a sunquake is still a topic of debate. However, Most authors agree that magnetic field re-structuring must play a fundamental role in causing such acoustic drivers. Previous studies have mainly probed the line-of-sight component of the magnetic field in such scenarios. In this work, we investigate the temporal and spatial evolution of permanent changes in the magnetic field geometry in a sample of five acoustically active flaring events using vector magnetograms acquired with the SDO/HMI instrument. The highly energetic events under study occurred during the past solar cycle 24, and cover a range of high and low GOES classes. The analysis carried out represents a crucial input for the investigation of sunquakes origin and dynamics.
The solar radio emission is usually divided into three parts depending of the time scale of the events: (1) the quiet Sun as a background emission, (2) a slowly varying component mostly associated with the active regions and (3) occasional extreme and sudden energetic phenomena like coronal mass ejections and flares. The quiet Sun emission comes from thermal bremsstrahlung in local thermodynamic equilibrium, therefore it has the advantage to be well understood and modeled compared to other frequencies.
The SunDish project aims to map and monitor the Sun at high radio frequencies with the Sardinia and Medicina Radio telescopes. In the framework of solar observations there is a lack of precise calibrated measurements in the K-band frequency range (18-26 GHz). We therefore perform observations in the K-band and in prospective we are going to extend our range up to 100 GHz.
In this work we present calibrated Sun maps by using the Supernova Remnant Cassiopeia A. This is a challenging procedure since this calibrator is an extended source and is currently in expansion. Due to its strong flux Cassiopeia A presents several advantages compared to other standard calibrators and its brightness variation is well study in literature. We find that Cassiopeia A is a very reliable calibrator for observations of the radio Sun. Due to the calibrator visibility at our telescopes latitude, it is possible to obtain accurately calibrated Sun maps throughout the day.
The solar radiation in the Lyman-alpha and Mg II h&k spectral lines plays a crucial role in the illumination of chromospheric and coronal structures, such as prominences/filaments, spicules, chromospheric fibrils, cores of coronal mass ejections, or solar wind. Moreover, it is important for the investigation of the heliosphere, Earth ionosphere, and the atmospheres of planets, moons, and comets.
We derived new sets of reference profiles of Lyman-alpha and Mg II h&k lines which describe the radiation from the solar disk during a minimum of solar activity. For the Lyman-alpha line, we used SOHO/SUMER raster scans obtained without the use of the SUMER attenuator while for the Mg II h&k lines we used the broad catalogue of IRIS full-Sun mosaic. We present here the reference profiles and their variation with the position on the solar disk and with the solar cycle. We also analyze how the change of the incident radiation influences the synthetic spectra produced by the radiative transfer modelling. The reference profiles data sets are published in Gunár et al. (2020) and Gunár et al. (2021).
We present a high fidelity snapshot spectroscopic radio imaging study of a weak type I solar noise storm which took place during an otherwise exceptionally quiet time. Using high fidelity images from the Murchison Widefield Array, we track the observed morphology of the burst source for 70 minutes and identify multiple instances where its integrated flux density and area are strongly anti-correlated with each other. The type I radio emission is believed to arise due to electron beams energized during magnetic reconnection activity. The observed anti-correlation is interpreted as evidence for presence of MHD sausage wave modes in the magnetic loops and strands along which these electron beams are propagating. Our observations suggest that the sites of these small scale reconnections are distributed along the magnetic flux tube. We hypothesise that small scale reconnections produce electron beams which quickly get collisionally damped. Hence, the plasma emission produced by them span only a narrow bandwidth and the features seen even a few MHz apart must arise from independent electron beams. These results, along with a few other works of similar nature, demonstrate the ability of spectroscopic snapshot imaging studies to detect these oscillatory phenomena. These studies have opened up a new phase space for detailed exploration of very weak/ low levels of activity.
On 21 February and 21-22 March 2021, the Extreme Ultraviolet Imager (EUI) onboard Solar Orbiter (SolO) observed three prominence eruptions. The eruptions were associated with coronal mass ejections (CMEs) observed by Metis, SolO's coronagraph. All three eruptions were also observed by instruments onboard PROBA2, SDO, STEREO-A and SOHO. An analysis of these eruptions is performed, together with the in-situ signatures of any associated interplanetary CME. We look in particular at their kinematics, direction of propagation and 3D reconstruction.
Like their larger counterparts, solar microflares release magnetic energy and accelerate particles to relativistic speeds. Even though they are generally shorter and often more compact than larger flares, they can display a surprising complexity and provide new insights into where and when particles are accelerated. Signatures of accelerated electrons are most readily observed at X-ray and radio wavelengths. We present observations of multiple electron acceleration sites and times during a series of solar microflares observed with the RHESSI X-ray instrument and at radio wavelengths with the Karl G. Jansky Very Large Array (VLA).
Multiple microflares were observed from the same active region over a period of 45 minutes. The VLA was observing the Sun during the same period at a time resolution of 50 ms at frequencies between 1 to 2 GHz. The radio dynamic spectra show a variety of features, like extremely short lived periodic spikes, drifting bursts, and broad band emission. While some of these emissions were temporally associated with X-ray sources, they originated from a different location. The observations suggest that, even in short, compact flares, acceleration of electron can take place at multiple locations, either co-temporally or at multiple instances during the course of the flare.
MHD plasma turbulence is believed to play a vital role in the production of energetic electrons during solar flares and non-thermal broadening of spectral lines is a key sign of this turbulence. Here, we determine how flare turbulence evolves in time and in space using spectral profiles of Fe xxiv, Fe xxiii and Fe xvi, observed by Hinode/EIS. Maps of non-thermal velocity are created for times covering the X-ray rise, peak, and decay. For the first time, the creation of kinetic energy density maps reveal where energy is available for electron energisation, suggesting that similar levels of energy may be available to heat and/or accelerate electrons in large regions of the flare. We find that turbulence is not localised in the loop apex but distributed throughout the entire flare; often greatest in the coronal loop tops, and decaying at different rates at various locations in the flare. For hotter ions (Fe xxiv and Fe xxiii), non-thermal velocity decreases as the flare evolves and after the X-ray peak, showing clear spatial variation decreasing linearly from the loop apex towards the ribbon. For the cooler ion, the non-thermal velocity remains relativity constant throughout the flare, but steeply increases in one region corresponding to the southern ribbon, peaking just prior to the peak in hard X-rays before declining. The results suggest that the turbulence has a more complex temporal and spatial structure than previously assumed, while the newly introduced turbulent kinetic energy maps help to identify important spatial inhomogeneities in the plasma motions.
Prediction of the future flare productivity of an active region (AR) when it is in the early-emergence stage is a longstanding problem. The aim of this study is to probe two parameters of the photospheric magnetic field, both derived during the emergence phase of an AR, and to compare them with the flare productivity of a well developed AR. The parameters are: (i) the index of the magnetic power spectrum (the slope of the spectrum) at the stage of emergence, and (ii) the flux emergence rate. Analysis of 243 emerging ARs showed that the magnetic power index increases from values typical of quiet-Sun regions to those typical of mature ARs within a day, while the emergence proceeds for several days; frequently, after the increase, the value of the power index oscillates around some mean value with the fluctuations being several times smaller than the growth of the power index during the emergence onset. For a subset of 34 flare-productive ARs we found no correlation between the power spectrum index at the stage of emergence and the flare index derived from the entire interval of the AR's presence on the disc. At the same time, the flux emergence rate correlates well with the flare index (Pearson's correlation coefficient is 0.74). We conclude that a high flux emergence rate is a necessary condition for an AR to produce strong flares in the future; thus the flux emergence rate can be used to probe the future flare productivity of an AR.
The Spectrometer/Telescope for Imaging X-rays (STIX) is a remote sensing instrument on-board the Solar Orbiter mission, conceived for the measurement of hard X-ray photons emitted by thermal and non-thermal mechanisms during solar flares. In particular, the scientific goal of STIX is to provide information on location, timing and spectrum of the accelerated electrons at the Sun. The STIX imaging concept is based on the Moire pattern technique that allows the measurement of 30 visibilities, i.e. Fourier components of the photon flux emitted during a solar flare. Hence, the imaging problem from STIX data is the one of reconstructing the flaring source by inverting a sparse sampling of its angular Fourier transform. In this talk we show the results obtained with several imaging techniques when applied to semi-calibrated or fully calibrated STIX visibilities. Specifically, we show the ability of Particle Swarm Optimization and Sequential Monte Carlo to solve a parametric imaging problem from visibility amplitudes alone, also giving quantitative estimates of the uncertainty of the reconstructed parameters. Moreover, we provide some insights about the calibration of the visibility phases and how imaging techniques can support the calibration process. Finally, we show the performances of maximum entropy and interpolation methods when applied to fully calibrated data. For assessing the validity of our results, we compare them to higher-resolution maps obtained by the Extreme Ultraviolet Imager (EUI) within Solar Orbiter, and the Atmospheric Imaging Assembly onboard the Solar Dynamics Observatory (SDO/AIA).
Two strong homologous white-light flares of GOES X-class occurred on the Sun on September 06, 2017. We describe the peculiarity of these events occurred in the super active region NOAA 12673, with a time interval, between their peaks, of about 3 hr. Using photospheric vector magnetograms, taken before the beginning of the two X-class events, as boundary conditions to reconstruct the non-linear force-free coronal magnetic field configuration, we identified two related 3D null points located at low heights above the photosphere (i.e. in very low corona). We deduce that their formation at such low altitudes may be ascribed to the strong and persistent shear motion of the main photospheric magnetic structures.
These events can be adopted as a hint for a possible interpretation of the activity of young G-type stars, recently reported by the Kepler mission. We argue that a possible explanation of the acceleration of huge numbers of particles producing white-light emission, during these events as during white-light flares in young Sun-like stars, might be attributed to the special accompanying conditions of the occurrence of magnetic reconnection at low altitudes in the stellar atmospheres.
The study of the localized plasma conditions before the impulsive phase of a solar flare can help us understand the physical processes that occur leading up to the main flare energy release. Here, we present evidence of a hot X-ray ‘onset’ interval of enhanced isothermal plasma temperatures in the range of 10-15 MK up to tens of seconds prior to the flare’s impulsive phase. This ‘hot onset’ interval occurs during the pre-flare time during which elevated soft X-ray flux is detected, but prior to detectable hard X-ray emission. The isothermal temperatures, estimated by the Geostationary Operational Environmental Satellite (GOES) X-ray sensor, and confirmed with data from RHESSI, show no signs of gradual increase and occurs regardless of flare classification or configuration. In a small sample of four representative flare events, we identify this early hot onset soft X-ray emission mainly within footpoint and low-lying loops, rather than with coronal structures, based on images from the Atmospheric Imaging Assembly (AIA) and the use of limb occultation. These hot X-ray onsets appear before there is evidence of collisional heating by non-thermal electrons, and hence challenges the standard flare heating modelling techniques.
Solar Wind streams, acting as a background, govern the propagation of coronal mass ejections in the heliosphere and drive geomagnetic storm activities. Therefore, predictions of the solar wind parameters are the core of space weather forecasts. Also, structure and dynamics of the heliospheric magnetic field (HMF) are key to understanding the solar wind flow. Typically, line-of-sight observations of a magnetogram is used to derive the HMF structure and then a solar wind model is used for forecasting solar wind parameters. Here, we present an implementation of our physics-based solar wind model aiming to compliment the in-situ measurements at 1 AU, in particular we will discuss our recent extension of the pilot study (Kumar et al., 2020) of data driven solar wind prediction at L1. We will demonstrate a detailed overview of our algorithm that incorporates coronal magnetic field modeling and the MHD approach adopted for inner heliosphere using PLUTO code. We will validate our results by comparing essential thermal and dynamical properties of solar wind at L1 and also discuss how these parameters are affected based on the choice of input magnetograms. Finally, we will associate the output of our 3-D physics-based approach to the observations from in-situ instruments at L1.
An assessment of the long-term behaviour of the solar wind is of paramount importance to understand the nature of its relationship with solar activity cycles, but also to evaluate its long-lasting effects on Earth. Understanding the long-term solar wind properties also helps putting in a different perspective space weather events on shorter time scales and extreme events. In order to connect the solar activity variations to solar wind properties, we used Ca II K index and solar wind OMNI data in the time interval between 1965 and 2020, which almost entirely covers the last 5 solar cycles. A time lag in the correlation between the parameters is found, that seems to show a temporal evolution over the different solar cycles. The results from our analysis offer the possibility to deepen the understanding of the processes that link the global dynamo to solar variability and to the properties of the solar wind near the Earth.
Coronal mass ejections (CMEs) are one of the major sources for space weather disturbances. If the magnetic field inside an Earth-directed CME or its associated sheath region has a southward-directed component (Bz), then it interacts effectively with the Earth’s magnetosphere, leading to severe geomagnetic storms. Therefore, it is crucial to predict the strength and direction of Bz inside Earth-impacting interplanetary CMEs (ICMEs) in order to forecast their geo-effectiveness. However, due to lack of realistic inputs and the complexity of the Sun-Earth system, it is difficult to perform reliable forecast of Bz at 1 AU.
In this work, using the observational properties of CMEs, we implement new techniques to constrain the kinematic and magnetic parameters of the analytical force-free flux rope model (spheromak) to mimic the magnetic structure of a CME and simulate its evolution from Sun-to-Earth using the “European heliospheric forecasting information asset” (EUHFORIA). In order to validate our tool, we simulate an Earth-directed CME event on 2013 April 11 and compare the simulation results with the in-situ observations at 1 AU. Both the field-strength and orientation of the ICME magnetic field vectors as obtained from the model show good agreement with that obtained from the in-situ observations. From the simulation results, we could also capture the overall magnetic structure of the associated sheath region ahead of the CME flux rope. The new techniques implemented in this study show promising results towards the forecasting of Bz in near real time.
Coronal Mass Ejections (CMEs) are triggered by kinetic-scale magnetic field topologies within the solar corona and evolve into large-scale structures with sizes of the order of the heliosphere itself. In this paper, we discuss the development of 3-D magnetohydrodynamic (MHD) simulations starting at the solar surface and extending outward through the solar corona and into the inner heliosphere. Using a force-free flux rope implementation in a magnetostatic corona, we are able to self-consistently capture the eruption of various flux rope orientations and subsequent interaction with pre-existing coronal environments. The accurate evolution is therefore highly sensitive to the initial environmental conditions and we demonstrate how the phenomenon of coronal and solar wind pre-conditioning can drastically impact a given CMEs characteristics. Accurately evolving flux rope CME structures beyond the corona presents a formidable modelling challenge and we discuss the advantages and draw-backs of using different CME descriptions for space weather forecasting.
Within the last years artificial intelligence (AI) excelled in many disciplines, providing major advances in image processing techniques with the use of deep learning. As part of the EU H2020 SOLARNET project we develop methods for the anticipated Solar Physics Integrated Network Group (SPRING), a global network of ground-based solar telescopes. In this presentation we discuss the application of deep learning to solar data, covering our recent developments and ongoing activities. We highlight three components of our data processing pipeline where AI can provide major advances. (1) We discuss the image pre-selection, where we developed a novel deep learning method for image quality assessment that is based on the true image distribution of high-quality observations and that provides an objective estimate that is in good agreement with the human perception. (2) For the post-processing of the observations we demonstrate the usability of image enhancement procedures and show that our deep learning approach can even mitigate strong atmospheric degradations (e.g., clouds), while solar features are preserved. (3) We discuss automated detection methods and focus on our newly developed solar flare and solar filament detection for Hα observations. We show that these deep learning methods can provide reliable detections in real-time and higher-level data products (catalogues) for further scientific use.
The Solar Activity Magnetic Monitor (SAMM) Network (SAMNet) is an international consortium of ground-based solar telescope stations. SAMNet, at its full capacity, will continuously monitor the intensity, magnetic and Doppler velocity fields at multiple heights in the solar atmosphere from the photosphere to the upper chromosphere. SAMM sentinels are equipped with a cluster of identical telescopes each with different magneto-optical filter (MOFs) to take observations in K~I, Na~D and Ca~I spectral bands. A subset of SAMM stations will also have white-light coronagraphs and emission line coronal spectro-polarimeters. The objectives of SAMNet are to provide data for space weather research and forecast. The goal is to achieve an operationally sufficient lead time of e.g. flare warning of 2-8 hours, and provide much sought-after continuous synoptic maps (e.g., LoS magnetic and velocity fields, intensity) of the lower solar atmosphere with spatial resolution limited only by seeing or diffraction limit, and with a cadence of 10-min. The individual SAMM sentinels link into their master HQ hub where data received from all the slave stations are processed and flare warning is issued up to 26 hrs in advance.
Solar energetic protons in solar cycle 24 accompanied by EUVI waves from SDO/AIA are analysed and presented. Multi-energy proton data from 10s to 130s MeV from the SOHO/ERNE instrument is used. Pearson and partial correlation analysis between the proton intensities and flare or CME parameters is performed. Additionally, the interplanetary conditions are inspected in terms of shock waves occurrence and large deviations from the nominal Parker spiral path. A comparison with the synthetic proton profiles in multiple energy bands produced with the new SPREAdFAST model (https://spreadfast.astro.bas.bg/) is performed and the results are discussed.
Comprehensive radiative MHD simulations of the solar atmosphere depend directly on few free parameters. However, the microphysics of the problem (including atomic and molecular data) is hidden in the opacity and equation of state used by numerical codes. We address the importance of various opacity contributors in 3D simulations of the solar photosphere done with the MANCHA code. This is critical for studies where highly accurate synthetic spectra are needed. For example, for solar irradiance variations (Criscuoli et al, 2020) or for abundance determinations.
We have developed a pipeline that starts with atomic and molecular data tables for computing monochromatic opacities using an open-source code (Synspec, Hubeny and Lanz, 2017), and finally constructs the opacity distribution function (ODF) and opacity bins that are used in convection simulations. We have run the MANCHA code, starting from the same initial state and for the same amount of solar time, with ODF and different numbers of opacity bins. The results of these runs are compared to test how accurately opacity binning approximates the full non-grey problem. In addition, we compare the results with similar simulations obtained using opacities produced by the ATLAS9 code (Castelli and Kurucz, 2003). Apart from analyzing the opacity bins and their influence on the temperature, we also compare the radiative output from snapshots (Fe I line and center-to-limb variation of the continuum). Having a well-tested and fully controllable pipeline for the opacity treatment is essential to extend MANCHA convection simulations to the case of other main sequence cool stars.
We study oscillations in the lower atmosphere of coronal hole regions, where the conditions are favorable for the propagation between the atmosphere layers. We analyse the features of the oscillations that show signs of propagation between the layers of the solar atmosphere. Using the cross-spectrum wavelet algorithm, we found that both chromospheric and photospheric signals under coronal holes share a range of significant oscillations of periods around 5 minutes, while the signals outside of coronal holes show no mutual oscillations in the photosphere and chromosphere. The phase shift between the layers indicates a predominantly upward propagation with partial presence of standing waves. We also tested the assumption that torsional Alfvén waves propagating in the corona originate in the lower atmosphere.
We used magnetic field data acquired by the Helioseismic and Magnetic Imager on board the Solar Dynamics Observatory to measure the magnetic flux decay rate in more than 800 active and ephemeral regions observed between 2010 and 2016. Our results suggest that for most active regions a power law between the peak magnetic flux and flux decay rate holds. At the same time part of unipolar active regions deviate from the common behaviour: these unipolar sunspots form a different flux decay rate versus peak flux distribution and exhibit sufficiently lower relative decay rate as compared to the rest of active regions. We suppose that there exists some mechanism that stabilizes unipolar active regions.
We investigate the three-dimensional distribution of the small-scale brightening events (“campfires”) discovered in the EUV quiet Sun by Solar Orbiter/EUI. We use a first commissioning data set acquired by the HRI_EUV telescope of EUI on 2020 May 30 in the 174 Å passband combined with the simultaneous SDO/AIA data taken in the similar 171 Å passband. The spatial resolution of the two telescopes is sufficient to identify the campfires in both datasets. The two spacecraft had an angular separation of around 31.5 degrees, which allowed for the three-dimensional reconstruction of the campfire position. These observations represent the first time that stereoscopy was achieved for brightenings at such a small scale. Manual and automatic triangulation methods were used. The height of campfires is between 1000 km and 5000 km above the photosphere, and we find a good agreement between the manual and automatic methods. The internal structure of campfires is mostly not resolved by AIA, but for a particularly large campfire we were able to triangulate a few pixels, which are all in a narrow range between 2500 and 4500 km. We conclude that the low height of EUI “campfires” suggests that they belong to the previously unresolved fine structure of the transition region and low corona of the quiet Sun. They are probably apexes of small-scale dynamic loops heated internally to coronal temperatures.
We present analysis of IRIS ultraviolet observations of cool loops visible after the maximum of M6.5 solar flare on June 22, 2015. The detailed investigation of the physical parameters and models of these loops was presented in Mikuła et al. (2017). The line profiles were modeled using Cloud Model and this allowed us obtaining the reliable physical parameters characterizing the moving plasma inside loops, e.g. velocity along the line-of-sight. Here we present the next step of the work - the reconstruction of the shape of the analyzed flare loops. The geometric method, that allows us to reconstruct the true shape of loops was introduced by Loughhead, Wang and Blows (1983). Based on the two-dimensional images of a given structure located on the solar disk or at the solar limb, we can obtain their true orientation and size. The shape of the analyzed loops was determined mainly from images obtained by IRIS, supplemented with SDO/AIA 171 ang. data in some cases. Using basic geometry and some assumptions we reconstructed geometrical parameters of the loop system and we could present them in three-dimensional space. Thanks to simple calculations based on method presented in Loughhead and Bray (1984) we could also get so-called true velocity of down-flow/up-flow of plasma, i.e. velocity along the axis of the loops. The obtained results for each loops were compared with the corresponding free fall velocities on the Sun.
The chromospheric inverse Evershed flow (IEF) transports material into sunspots along the magnetic field lines that connect the boundary of the moat cell with the outer penumbra. In this study, we combine high-resolution observations of NOAA 12418 taken from the Dunn Solar Telescope and magnetic field measurements from the Helioseismic and Magnetic Imager (HMI) to investigate the driver of the IEF. We use the spectra of H$\alpha$ and Ca II IR to derive the chromospheric line-of-sight velocities, while the HMI magnetograms are used as an input to non-force-free magnetic field extrapolation to track closed magnetic field lines (MFLs) near the sunspot in the active region. This allows us to determine their length and height, locate their inner and outer foot points and derive flow velocities along them. We find that the MFLs related to the IEF reach on average a height of 3 Mm over a length of 13 Mm and the inner and outer foot points are located at 1.2 and 1.9 sunspot radii respectively. The average field strength difference $\Delta B$ between inner and outer foot points is around 400 G, which is anti- correlated to the temperature difference $\Delta T$, which has an average value around -100 K. This leads to an average pressure difference of 2 kPa. We conclude that the IEF is driven along magnetic field lines connecting network elements with the outer penumbra by a gas pressure difference that results from a difference in field strength as predicted by the classical siphon flow scenario.
Since the hint of the existence of an invariable value of the vertical magnetic field (Bver) on umbra-penumbra boundaries in sunspots by Jurčák (2011), many investigations have focused on studying this property. Umbra-penumbra boundaries of stable sunspots are defined by a critical Bver (Jurčák et al. 2018, Schmassmann et al. 2018; Lindner et al. 2020). On the other hand, when an umbra or pore do not hold a sufficiently strong Bver, i.e. the inclined field is weaker than the critical value, penumbral magneto-convection overtakes (Jurčák et al. 2015; Jurčák et al. 2017). Here we introduce the study of an evolving pore that does not develop a penumbra. We find a stable phase where the pore does not significantly change and the Bver on its boundary reaches a maximum value, comparable to the critical value found on umbra-penumbra boundaries. We call this value the critical vertical field of the pore. The evolution is complex, however, we find that regions of the pore defined by the critical value are more stable during the first period of the decay. Afterwards, when the pore is separated into smaller patches, the segments with strong Bver decay at the same rate as the whole area of the pore. This study suggests the existence of a critical value of Bver that hinders magneto-convection in pores as well. In addition, in this case study, the stable regions of the pore can be similarly well defined by a critical value of the total magnetic field strength.
We present the analysis of spectropolarimetric data obtained with the CRISP instrument at the SST in the Ca II 845.2 nm line. We used the Weak-field approximation (WFA) to obtain information about the magnetic field present in chromospheric spicules and coronal rain clumps. Albeit being computationally simple to implement, to correctly apply the WFA requires a careful assessment of the conditions of the plasma. Magnetic fields of the order of hundreds of Gauss were inferred in a large number of spicule and coronal rain pixels. In the later case, the full magnetic field vector could be determined. We also combined simultaneous Ca II 845.2 nm and Hα intensity observations to estimate the temperature and non-thermal velocity of the plasma in coronal rain and spicules. The statistical distribution of the temperature of spicules (coronal rain) peaks at 15,000 K (20,000 K) and the microturbulent velocity lies in the range 5-20 km/s (0-15 km/s) and peaks at 12 km/s (5 km/s).
From more than 60 years of observations, we have known that the inner solar corona has low-density plasma structures called coronal holes (CHs). Since CHs appear to be connected to the sources of high-speed solar wind streams, which in turn are typically linked to geomagnetic storms, their study is of particular relevance in the field of Space Weather.
The connection between the photospheric magnetic field and the CHs has been studied for the same time. Compared to other regions of the corona, photospheric magnetic fields associated to CHs have a dominant magnetic polarity which results in magnetic field lines that do not close in the proximity of the Sun.
To investigate the statistical properties of the photospheric magnetic field underlying CHs and “normal” coronal regions a classical technique, the signed measure, is used. This technique allows to characterize the scaling behavior and the topology of sign-oscillating magnetic structures in selected regions of SDO/HMI LoS magnetograms.
To this end we have compared the properties of the photospheric magnetic field underlying 60 CHs and 60 non-coronal holes (non-CHs). In particular, in addition to having studied distributions and momenta of photopsheric magnetic fields associated to the selected regions, we have performed the sign singularity analysis computing the cancellation functions of the highly fluctuating photospheric magnetic fields.
Here we present the results of the analysis on the 120 sub-regions extracted from the SDO/HMI magnetograms highlighting the recurrences in the emergence scales of the sign imbalance in CHs compared to non-CHs.
UV compact bursts (CBs) are observed by IRIS in both NUV and FUV channels. They appear as small and intense short lifetime brightenings visible in solar active regions. Some of them can be connected with well-known Ellerman bombs and IRIS bombs.
Our interest in CBs was initiated by the paper published by Grubecka et al. (2016), in which we modelled 5 different selected CBs observed in Mg II h and k lines. Next goal is to investigate statistical diversity of Mg II h and k lines of CBs and their visibility in far UV lines such as Si IV, C II and in Mg II triplet. In order to achieve goals, in IRIS database we searched for dense rasters of active and emerging flux region containing spectra in Mg II, C II and Si IV. Next step was to create spectroheliogram for each raster in which we were searching for CBs with the size of the order of 1''.
We performed survey of 2053 CBs using some of the parameters of the Mg II k line profile: contrast in characteristic profiles points and FWHM. We used also some parameters of Si IV, C II and Mg II UV triplet lines. This analysis allows us to categorize CBs as in Grubecka et al. 2016. We also have searched for correlations between the emission in Mg II lines and hotter Si IV line in order to find which of events are linked to IRIS bombs, UV burst or Ellerman Bombs.
We simulate transverse oscillations in radiatively cooling coronal loops and forward-model their spectrometer and imaging observations, paying attention to the influence of background emission. The transverse oscillations are driven at one footpoint by a periodic velocity driver. A standing kink wave is subsequently formed and the loop cross-section is deformed due to the Kelvin-Helmholtz instability, resulting in energy dissipation and heating at small scales. Besides the transverse motions, a long-period longitudinal flow is also generated due to the ponderomotive force induced slow wave. We then transform the simulated straight loop to a semi-torus loop and forward-model their spectrometer and imaging emissions, mimicking observations of Hinode/EIS and SDO/AIA. We find that the oscillation amplitudes of the intensity are different at different slit positions, but are roughly the same in different spectral lines or channels. X-t diagrams of both the Doppler velocity and the Doppler width show periodic signals. We also find that the background emission dramatically decreases the Doppler velocity, making the estimated kinetic energy two orders of magnitude smaller than the real value. These results are helpful for further understanding transverse oscillations in coronal loops and their observational signatures, but also cast doubt on the spectroscopically estimated energy content of transverse waves using the Doppler velocity.
We present a statistical analysis of power distribution of oscillations in plage of the active region NOAA AR12651, observed jointly with ALMA, IRIS, and AIA. We employ coordinated ALMA Band-6 (1.25 mm) brightness temperature maps, IRIS images in 2796 Å passband, and observations in six AIA passbands (1600 Å, 304 Å, 131 Å, 171 Å, 193 Å, and 211 Å). We study the spatial association of oscillations over the atmosphere mapped by these different passbands, focussing on the correlation of power distribution of ALMA oscillations with others. We do not observe any significant association of ALMA oscillations with IRIS and AIA oscillations. The spatial distribution of dominant periods and power in different period intervals of ALMA oscillations is observed to be uncorrelated with any other passband. We attribute the non-association of ALMA oscillations with those of IRIS and AIA to the significant variation in the height of formation of the millimeter continuum observed by ALMA.
The validity of the lambda-meter method for determining the quiet Sun velocity field using the Si I 1082.7 nm line is investigated. To this end, the intensity profiles of this line were calculated for the solar disk center by means of NLTE simulations in a three-dimensional model atmosphere describing the small-scale magnetic activity in the quiet solar photosphere. The velocity field recovered using the lambda-meter method from theoretical NLTE profiles of the Si I 1082.7 nm line was compared with the velocity field from the model atmosphere. The influence of atmospheric and instrumental effects on the results is considered. These effects are atmospheric turbulence and light diffraction by telescope aperture, such as VTT, GREGOR, and EST/DKIST. It is shown that in the case of observations of the Si I 1082.7 nm line on large-diameter telescopes like GREGOR and EST/DKIST with a spatial resolution substantially better than 0.27″, the lambda-meter method provides reliable values of the velocity field for the lower and upper solar photosphere. For the middle photosphere, the correlation between the inferred and the real velocities is worse, particularly when using the smaller diameter telescopes like VTT. Under a poor spatial resolution exceeding 2″, information about the velocity field can be obtained only for the uppermost photospheric layers. For this case, the lambda-meter velocities turn out to be noticeably smaller than the real values.
Solar magneto-seismology (SMS) is a popular research area that involves the study of MHD waves and oscillations present in structures of the magnetized solar atmosphere. Magnetically confined features such as magnetic slabs or flux tubes are important aspects that have been studied in great detail for more than a decade. Inhomogeneities in the structuring of the magnetic field enables them to act as wave-guides for a variety of the MHD wave modes. A flux tube with a cylindrical core surrounded by a magnetic shell is a good initial model capturing inhomogeneities observed in solar atmospheric waveguides. We investigate standing ideal MHD waves in the magnetic annulus geometry. We consider an annular cylinder of fixed length with appropriate line-tying boundary conditions to derive a dispersion relation for the sausage and kink MHD modes. We find analytical solutions to the dispersion relation by considering the weakly homogeneous flux tube (WHFT) and thin annulus approximations (TAA). Further, we also consider the wide and thin flux tube cases and apply our results to solar magnetic loops from lower atmospheric oscillations (sub-photospheric tubes and chromospheric fibrils) to coronal loops. We find, in general, two purely surface and two body mode solutions in the considered structuring that we use then to determine the period ratio of the fundamental and first excited harmonic, for SMS purposes. We analyze the role of annular structuring on the period ratios of standing waves and discuss its importance in the context of solar magneto-seismology.
The solar wind is a stream of charged particles originating from the Sun and interacting` with Earth’s magnetic field. Any alterations in the solar wind affects Earth’s magnetic field and can cause geomagnetic storms. Thus, understanding the formation and acceleration of the solar wind is critical towards investigating the Sun-Earth connection and predicting space weather.
The solar chromosphere is a dynamic layer is filled with many features that vary in time and space. In this project we focus on plasma dynamics of jets observed along the coronal hole boundary. The interaction of these events with the neighboring plasma can influence solar wind.
We aim to address the questions:
A.1) What physical processes create upward propagating jets on coronal hole boundaries?
A.2) What physical processes are responsible for the acceleration and creation of jet turbulence?
We present a statistical study of jets formed along coronal hole boundaries. Jets can transfer mass and energy along open magnetic field lines and reach the solar wind. We investigate oscillations of different motions using CRISP (SST). We classify these oscillations as high-frequency (>5 mHz) and low frequency (<5 mHz) regions, and then investigate different waves that flow around the jets. We show whether such jets are observed in IRIS and SDO channels in higher solar atmospheric regions. We show how the morphology of the jets vary across the solar atmosphere and in future work, we will show how plasma properties change, to quantify their role as mass and energy channels that could accelerate solar wind.
We analyze the coronal elemental abundances during a small flare using Hinode/EIS observations. Compared to the preflare elemental abundances, we observed a strong increase in coronal abundance of Ca xiv 193.84 Å, an emission line with low first ionization potential (FIP < 10 eV), as quantified by the ratio Ca/Ar during the flare. This is in contrast to the unchanged abundance ratio observed using Si x 258.38 Å/S x 264.23 Å. We propose two different mechanisms to explain the different composition results. First, the small flare-induced heating could have ionized S, but not the noble gas Ar, so that the flare-driven Alfvén waves brought up Si, S, and Ca in tandem via the ponderomotive force which acts on ions. Second, the location of the flare in strong magnetic fields between two sunspots may suggest fractionation occurred in the low chromosphere, where the background gas is neutral H. In this region, high-FIP S could behave more like a low-FIP than a high-FIP element. The physical interpretations proposed generate new insights into the evolution of plasma abundances in the solar atmosphere during flaring, and suggests that current models must be updated to reflect dynamic rather than just static scenarios.
We propose the new approach in which the elemental plasma composition can be determined simultaneously with the distribution of differential emission measure (DEM). For this purpose we use the differential evolution (DE) method. We investigate the abundances of K, Ar, S and Si and DEM distributions for the flare on 21 January 2003 observed by RESIK in the soft X-ray range. Before applying the DE to the analysis of real observations we performed numerous tests of its usefulness. The results of these tests as well as the abundances of elements determined for the 21 January 2003 flare will be presented and discussed.
The presence of multiple current sheets in reconnection environments is expected due to the inherent turbulence associated with it. A velocity shear in reconnection environments is also common due to the dynamic nature of the process. We have investigated the effect of a sub and super-Alfvenic velocity shear on the explosive phase of an “ideal” double tearing mode (DTM) within the 2D resistive magnetohydrodynamic framework. The system exhibits an explosive reconnection phase which is a combined result of the plasmoid instability and an island structure driven instability where the cascading effect of the magnetic islands tend to increase the reconnection rate by pushing magnetic flux towards the x-points. We find that the theoretical scaling of the reconnection rate in the presence of a velocity shear flow is strongly dependent on the island half-widths and larger sized islands tend to enhance the reconnection rate drastically. These types of scaling in explosive systems evolving on an “ideal timescale” are relevant from the perspective of magnetic reconnection in very high Lundquist number systems such as those realized in the solar corona.
Simultaneous spectroscopic and imaging observations can provide deep insight into diagnostic parameters of the solar corona and help us to understand the dynamics and origin of coronal mass ejections(CMEs). Visible emission line coronagraph (VELC), a payload on-board Aditya-L1, will provide spectroscopic observations of the inner corona from 1.05 R$_\odot$ to 1.5 R$_\odot$ in pass-bands corresponding to three ionization states of iron, FeXIV (5303 $A^\circ$), Fe XI (7892 $A^\circ$), and FeXIII (10747 $A^\circ$) and imaging in white-light continuum channel from 1.05 R$_\odot$ to 3 R$_\odot$. To understand the instrument performance before its launch, we have used CHIANTI atomic database to generate synthetic spectra for the spectral channels in the temperature range of 1 MK to a few MK. We added the synthetic spectra with instrument scattered photon noise and detector noise and investigated the impact of plasma temperature on the signal-to-noise ratio (SNR). The SNR found to be highest at the formation temperature of the lines. We simulated synthetic spectra for a CME which was observed by KCor. The increment was seen in the peak electron counts for all three channels in the presence of CME. Doppler velocity was imposed on spectra of 5303 $A^\circ$ at 1.4 R$_\odot$ for different SNR values and recovered after adding random noise to the spectra. The recovered Doppler velocity showed a notable departure from the imposed one for SNR $\approx$1 at line peak. In this poster, I will present the impact of different solar conditions on the performance of the spectral channels of VELC.
With the advent of modern compact radio interferometric arrays in metrewavebands, high fidelity snapshot spectroscopic imaging studies at sub -second and sub-MHz scales became possible. Murchison Widefield Array (MWA) operating in 80 - 240 MHz band is one such array. A recent study using MWA data of a radio burst source, associated with a microflare, discovered correlated quasi-periodic pulsations in its size, orientation and flux with a dominant periodicity of 30s. Two modes of correlated evolution were also discovered in the burst source evolution: S and T modes. The S mode showed anti-correlated QPPs in the size and flux, akin to a sausage mode. But, the T mode had correlated QPPs in the size and orientation, like a twist-untwist motion. The 30s periodicity could be linked to local Alfven timescale across the dominant magnetic field braids in the system. T mode QPPs were found in the pre-flare phase, while during the microflare S mode came into prevalence alongside the T mode. In the post-flare phase, T mode paved way completely to S. This flare mediated mode conversion from T to S possibly relates to the redistribution of excess free energy in the critically braided pre-flare magnetic loop. Understanding these modes and their evolution could serve as a diagnostic for probing physical dynamics at weak particle acceleration/flaring events, which are often difficult to study using high energy observations.
We present a catalogue of plasma jets in the solar corona with a temperature above 0.5 MK. The catalogue contains primary information about the event and of the parameters of the jet, based on the data obtained with the spaceborne high-precision EUV imaging telescope SDO/AIA and ground-based radio telescopes and spectrometers, including RATAN-600 (Radio telescope of the Russian Academy of Sciences, Russia), SRH (Siberian Radio Heliograph, Russia) and NoRH (Nobeyama Radio Heliograph, Japan). To obtain the primary parameters of the jets, we developed a new method of automatic jet detection in homogeneous time series of images. For some events, the catalogue is complemented with data on the reconstructed magnetic field. The purpose of the catalogue is to provide summary information about coronal jets to all interested researchers for further statistical analysis, determination of characteristic parameters of jets, and in-depth study of individual events. Currently, the catalogue covers the time interval from 2010 to 2019, and the data is continuously added. The work was supported by the Russian Foundation for Basic Research grant No. 18-29-21016.
Since the discovery of the solar corona, many attempts have been made to model its behaviour. Perhaps the most well-known attempt was made by Parker (1958) when he assumed that the quiet sun corona is in hydrodynamical balance. Nevertheless, his model has several limitations (a saddle point, non-diverging solutions, etc). Lemaire & Stegen (2016) introduced the DYN model that addressed those issues by assuming a more realistic electron density distribution and boundary conditions based on in-situ observations at 1 AU.
More recently, Lemaire & Katsiyannis (2021) expanded further on the DYN model and produced electron temperature profiles, $T_e(r)$, for a variety of observed conditions. They found a very large increase in $T_e(r)$ at radial distances of ~2-5 solar radii and conjectured that a heating process takes place at those levels.
This contribution will present the DYN model, with its assumptions and limitations. It will also contain the most important results published by Lemaire & Stegen (2016), and Lemaire & Katsiyannis (2021), including temperature profiles for a variety of commonly observed conditions. A comparison between the $T_e(r)$ predictions of the model and recent observations will also be included. Finally, there will be a discussion about future work and the reduction of the number of assumptions.
The Ca II 854.2 nm line is currently one of the most favored spectral lines for spectropolarimetric studies of the solar chromosphere. The interpretation of the line is commonly supported by sophisticated NLTE inversion codes, which look for the atmospheric stratification whose Stokes profiles best match the observed data. Several studies have employed this line to analyze oscillatory phenomena in sunspots, such as umbral flashes. Umbral flashes are sudden brightenings in the core of the line produced by the propagation of waves coming from photospheric layers and developing into shocks. In this work, we evaluate the potential of the Ca II 854.2 nm line for studying chromospheric oscillations in umbrae. We have developed numerical simulations of wave propagation in a sunspot. The Stokes profiles emerging from these models have been computed using the NLTE code NICOLE. We have compared the oscillations in velocity, temperature, and magnetic field inferred from the inversions of the synthetic profiles with the original oscillations. The chromospheric velocity and temperature oscillations are reasonably captured by the inversions since the output models reproduce their amplitude and main period. Their power spectra exhibit a secondary power peak, possibly due to fluctuations in the formation height of the line. The inferred magnetic field shows spurious fluctuations with peak-to-peak amplitude around 300 G, which is absent in the original data. Our results support the use of the Ca II 854.2 nm line for the analysis of chromospheric waves, but suggest caution with the interpretation of oscillations in the magnetic field.
The ubiquity of low-amplitude decayless kink oscillations of plasma loops allows for the seismological probing of the corona on a regular basis. We analysed decayless kink oscillations in several distinct loops belonging to active region NOAA 12107 during its quiet time period. The oscillation periods were estimated with the use of the Motion Magnification technique. The lengths of the oscillating loops were determined within the assumption of its semicircular shape by measuring the position of their footpoints. The density contrast was estimated from the observed intensity contrast accounting for the unknown spatial scale of the background plasma. The combination of those measurements gives the distribution of kink and Alfvén speeds in the active region. Thus, we demonstrate the possibility of obtaining seismological information about coronal active regions before flares and CMEs, which can be used for their forecasting. Using full 3D magnetohydrodynamic numerical simulations, we studied the effects of magnetic field sigmoidity on the fundamental kink oscillation. Our model consists of a single denser coronal loop, embedded in a plasma with dipolar force-free magnetic field with a constant α-parameter. For a loop with no sigmoidity, we find that the numerically determined oscillation period matches the theoretical period calculated using WKB theory. With increasing sigmoidity, the actual period is increasingly smaller than the one estimated by WKB theory. The discrepancy could be exploited seismologically to determine the free energy in the hosting active region.
Whistlers can be important both for electron transport in flaring loops and for electron scattering in acceleration sites. In this talk we focus on two questions: how accelerated electrons generate whistlers in a flaring loop and how the initial electron energy spectrum is transformed due to interactions with the whistlers. It is shown that for a given non-stationary injection of nonthermal electrons, all three regimes of turbulent diffusion, weak, moderate, and strong, can be realized simultaneously but in different energy domains. It is found that the reverse action of the generated whistler turbulence significantly changes characteristics of the spatial, temporal, pitch-angular and energy distributions of electrons. In particular, the energy spectrum of electrons in the range 30 keV - 10 MeV can undergo transitions from hard to softer and again to harder. Besides of this, the electron spectrum undergoes some specific temporal changes. The obtained results can be of great importance for microwave, hard X-ray, and gamma-ray diagnostics of solar and stellar flares.
We study quasi-periodic oscillations of two solar filaments based on observations in 304 \AA ultraviolet line provided by SDO/AIA.
Time-distance diagrams based on the intensity maps were produced. Quasi-periodic oscillations of the transverse dimensions of the filaments with periods of 4-8 and 10- 20 minutes have been revealed. On the basis of the obtained results, the amplitude-phase relations between the changes in the intensity and the transverse dimensions of the filaments are discussed.
This work was supported by the Russian Foundation for Basic Research grant # 20-52-26006, and the Ministry of Education and Science (NIR no. 0831-2019-0006).
We present high-resolution and multiline spectropolarimetric observations of a C2-class solar flare (SOL2019-05-06T08:47). The rise, peak, and decay phases of the flare were recorded continuously and simultaneously in the Ca II K, Ca II 8542 Å, and Fe I 6173 Å lines with the CRISP and CHROMIS instruments at the Swedish Solar Telescope. At the flare footpoints, a non-LTE multiline inversion code (STiC) was employed to infer the temperature, magnetic field, line-of-sight (LOS) velocity, and microturbulent velocity. All observed lines were analyzed simultaneously in order to understand the stratification of the physical parameters in the flaring and non-flaring atmosphere. In this talk, we will discuss the temporal behavior of the inferred parameters during flare and non-flare times in the photosphere and the chromosphere. Moreover, the LOS magnetic field changes in the photosphere and the chromosphere during the flare. We will also discuss how our less intense C-class flare can heat the deeper layers of the solar chromosphere, mainly at the flare footpoints, without affecting the photosphere.
In the standard eruptive flare model, magnetic reconnection originates in a thin current sheet; created by the inflow of oppositely orientated magnetic fields under a rising magnetic flux rope. The current sheet is notoriously difficult to observe directly, primarily due to the small size of the region. However, insights into current sheet dynamics can be revealed by the behaviour of flare ribbon substructure, as magnetic reconnection accelerates particles down reconnected field lines to the chromosphere to mark the flare footpoints. Behaviour in the ribbons can therefore potentially be used to probe processes occurring in the current sheet. Motivated by a similar study on the Earth's magnetosphere (Kalmoni et al 2015, 2018), we exploit this magnetic connectivity between the current sheet and magnetic footpoints to probe for signatures of waves and instabilities at the current sheet during the pre-impulsive phase of a small B-class solar flare (Jeffrey et al 2018). We use Fast Fourier Transforms of high-cadence (1.7 s) IRIS slit-jaw observations, back mapping observed spatial frequency scales and growth rates to the reconnection site. We compare these parameters to those expected from theoretical current sheet processes, such as the tearing mode or Kelvin-Helmholtz instabilities. This provides an observational constraint (for a single flare case-study) on the current sheet processes contributing towards the small-scale breakdown of ideal MHD needed to trigger the onset of fast magnetic reconnection on the Sun.
The chromospheric hydrogen Lyman-alpha line at 1216A is the brightest emission line in the solar spectrum, and yet studies of solar flares at this wavelength have been scarce in the recent literature. Changes in the Sun’s Lyman-alpha output can drive changes in the dynamics and composition of planetary atmospheres, and Lyman-alpha is also a significant radiator of solar flare energy providing an important diagnostic of energy release and transport processes. Milligan et al. (2020) published a statistical study of ~500 M- and X-class flares using GOES/EUVS data, showing that although the Lyman-alpha irradiance increases by only a few percent during large events, it can radiate up to 100 times more energy than the corresponding X-rays. Flares that occurred closer to the solar limb, however, were found to exhibit a smaller Lyman-alpha enhancement relative to those on the disk due to opacity and/or foreshortening effects. It was also shown that acoustic oscillations in the chromosphere can be detected through Lyman-alpha flare observations, and that impulsive Lyman-alpha emission, not X-rays, can induce currents in the E-layer of Earth’s ionosphere. A follow-up study included B- and C-class flares (Milligan 2021), which although not readily observable in disk-integrated measurements, can be investigated using a superposed epoch analysis. Despite increases of <1% above the solar background, a clear centre-to-limb variation was found in agreement with larger events. These findings should serve as a baseline for the advent of new Lyman-alpha flare observations and advanced numerical simulations that will become available during Solar Cycle 25.
ASPIICS/Proba-3 is a giant white-light coronagraph developed by ESA and will be launched in mid-2013. Proba-3 will consists from two satellites flying synchronously, the first one carrying the external occulter (EO) and the second one ~150 behind, carrying the optical telescope. The telescope will be placed in the shadow of the EO with high accuracy. The coronagraph is equipped with a filter wheel (3 spectral filters, 3 linear polarizers), a multi-exposure regime with provisional exposure times 0.1 s, 1.0 s and 10.0 s, is foreseen.
The on-ground processing of the registered data will include correction of all the instrument-related effects such as stray light, detector dark current and bias, perform radiometric calibration, include further processing steps – merging of different exposure times, retrieval of polarized data products, separation of signal in spectral lines.
Our initial aim was to prepare test data for validation of the processing algorithms. For this we have developed a physical model/software which takes into account all the known effects: we start with input coronal images and “propagate” them down to the detector taking into account diffraction, scattering and ghost light, total optical throughput, detector performance (quantum efficiency, nonlinearity, gain, dark current), and introduce noises based on their physical mechanisms.
The developed model allowed us to better understand performance of the coronagraph, estimate its radiometric sensitivity, analyze potential influence of random noise and systematic uncertainties. We analyze signal-to-noise ratio and propose optimized exposure times.
We present the model and discuss main characteristics of the coronagraph.
The Lyman Continuum (LyC; 912Å) is the free-bound transition of a free electron to the ground state of an ambient Hydrogen nuclei. LyC has been shown to be a powerful tool for probing the chromospheric plasma conditions during solar flares. By fitting the LyC spectrum, the departure coefficient of hydrogen, b1, and the colour temperature, Tc, can be determined. Where b1 is a measure of the degree of local thermodynamic equilibrium of a plasma and has been observed to approach unity during flares. When b1 approaches unity, Tc is approximately equal to the electron temperature of the plasma. Observationally, Tc has been observed to increase more at shorter wavelengths during some events suggesting the existence of an optically thin component of LyC at higher altitudes than the optically thick component. We have been analysing LyC profiles from a grid of 1D radiative hydrodynamic RADYN models hosted by QUB that were generated as part of the F-CHROMA project. These model atmospheres were generated for a range of nonthermal heating functions, based on characteristic electron fluxes, spectral indices, and low-energy cutoffs. From the models, we are investigating the temporal evolution of b1 and Tc in response to a range of heating functions. By generating contribution functions for these flare models, we will probe the height at which LyC forms in the solar atmosphere, and under what conditions, with the aim of comparing our predictions with LyC observations from the EUV Variability Experiment on board the Solar Dynamics Observatory.
Type II solar radio bursts are believed to be caused by magnetohydrodynamics (MHD) shock-accelerated electrons in the solar corona. Often type II radio bursts can display fine structure in dynamic spectra. However, the cause of this fine structure and its relation to the shock is currently unclear. Here we present results from imaging analysis of type II radio burst fine structures observed by the Murchison Widefield Array (MWA) on 2014-Sep-28. The MWA provides high-sensitivity imaging spectroscopy in the range of 80-300 MHz with a time resolution of 0.5 s and frequency resolution of 40 kHz. We examine the small-scale motion of type II fine structure radio sources in MWA images. We suggest that this small-scale motion may arise due to propagation effects, a combination of scattering and refraction from coronal turbulence, and not because of the physical motion of the shock location. The study of the systematic and small-scale motion of fine structures may therefore provide a measure of turbulence in different regions of the shock and corona. We discuss how imaging the fine structure in type IIs can be used as a probe of propagation effects and turbulence during shock propagation through the corona.
The solar wind is frequently perturbed by transient structures (magnetic folds, jets, waves and flux-ropes) that propagate away from the Sun over a large range of heliocentric distances. Parker Solar Probe has detected a large number of these at small heliocentric distances, together with surprisingly large solar wind rotation rates. Sun-to-spacecraft connectivity analysis shows that a large fraction of the corresponding solar wind flows were formed and accelerated in the vicinity of polar coronal hole boundaries.
We show via global MHD simulations that coronal rotation is highly structured in proximity to those boundary regions, in agreement with SoHO/UVCS synoptic observations and possibly with future Solar Orbiter/Metis campaigns. Enhanced poloidal and toroidal flow shear and magnetic field gradients also develop on such boundaries, and some regions can develop field-aligned and/or transverse vorticity. Some of these wind shears are noticeable tens of solar radii away from the surface, and therefore have a potential impact on the propagation of such magnetic perturbations across extended heights in the solar wind. We conclude that these regions of persistent shears are undoubtedly sources of complex solar wind structures, and suggest that they can trigger instabilities capable of creating magnetic field reversals detected in-situ in the heliosphere.
Our simulations furthermore indicate that the spatial structure of the solar wind shear will become more complex as the solar cycle progresses, with strong and extended shears appearing at heliographic latitudes that will be probed by Solar Orbiter in the near future.
Despite studying the kinematics of Coronal Mass Ejections (CMEs), the main challenges faced in this area are due to projection effects and lack of information in the inner corona. We have tried to improve on these shortcomings by implementing the Graduated Cylindrical Shell (GCS) model to the pair of images taken by COR-1 and COR-2 on-board STEREO-A/B, and studied their initial 3D evolution. Combining 3d profiles of width evolution and acceleration, we found observational evidence that the impact of Lorentz force on the CME kinematics, stays dominant till a height range of 2.5-3 R. We further found from a statistical perspective, that the kinematics in the outer corona is strongly coupled by the kinematics in the inner corona. With the upcoming solar missions that are dedicated to inner coronal observations, the results of our work focuses on exhibiting the significance of inner corona for a complete understanding of CME kinematics.
Ionospheric ions (mainly H+, He+ and O+) escape from the ionosphere and populate the Earth’s magnetosphere. The ionospheric population is variable, and it makes significant contributions to the magnetospheric mass density in key regions where magnetic reconnection is at work. Solar wind – magnetosphere coupling occurs primarily via magnetic reconnection, a key plasma process that enables transfer of mass and energy into the near-Earth space environment. Reconnection leads to the triggering of magnetospheric storms, auroras, energetic particle precipitation and a host of other magnetospheric phenomena. Several works in the last decades have attempted to statistically quantify the amount of ionospheric plasma supplied to the magnetosphere, including the two key regions where magnetic reconnection occurs: the dayside magnetopause and the magnetotail. Recent in-situ observations by the Magnetospheric Multiscale spacecraft and associated modeling have advanced our current understanding of how ionospheric ions alter the magnetic reconnection process, including its onset and efficiency. We review the current understanding of the ionospheric plasma supply to the magnetosphere and discuss the main implications for solar wind - magnetosphere coupling. The magnetopause can be significantly mass-loaded only during disturbed magnetosphere conditions, when the ionospheric ion production is enhanced, and the efficiency of the reconnection process is reduced. In addition, the multi-component nature of the ionospheric populations modifies how magnetic reconnection proceeds at kinetic scales most of the time, although the implications of these changes for the global efficiency of the coupling are not well understood.
Magnetic clouds are large-scale transient structures in the solar wind with low plasma β, low-amplitude magnetic field fluctuations, and twisted field lines with both ends often connected to the Sun. We analyse the normalised cross helicity, σc, and residual energy, σr, in magnetic clouds observed at sub-1 au heliocentric distances by Parker Solar Probe (PSP), and compare to clouds observed at 1 au by the Wind spacecraft. Magnetic clouds commonly display low values of |σc|, indicating that the Alfvénic wave flux parallel and anti-parallel to the mean field is approximately balanced. This low |σc| is likely caused by the closed field structure of magnetic clouds, and is in contrast to the generally higher |σc| found on the open field lines of the solar wind. These properties are compared to those found in the compressed and heated sheath regions upstream of the clouds: sheaths tend to have more solar wind-like turbulence properties.
To better understand the solar wind dynamic interactions with Coronal Mass Ejections (CMEs), we examine the effect of magnetic erosion on to the well-known aerodynamic drag force acting on CMEs. In particular, we consider the interplay between reconnection with the ambient solar wind and the virtual mass component of the drag equation. We quantify the effect of magnetic reconnection, which erodes part of the CME mass and magnetic flux, on the drag acting on CMEs and, eventually, we determine its impact on the time and speed of arrival of CMEs at 1 AU.
The nature of the slow solar wind, continuous or intermittent flow, is still debated; coronagraphs and heliospheric imagers regularly observe a spectrum of transient slow wind flows; e.g. instance blobs, jets. etc. A standard tool for the study of such flows, is the display of intensity as a function of time and elongation along a given direction, which is called a J-map. The launch of the Parker Solar Probe (PSP) mission in 2018, and the availability of high-quality up-close images of the corona by its Wide-Field Imager (WISPR) opened new exciting observational capabilities in solar wind research. Here, we report on simulations of synthetic WISPR J-maps constructed for various scenaria of transient solar wind release in terms of blobs. The methodology is based on Monte-Carlo simulations of blobs with varying numbers, release frequencies, speeds, and launch longitudes. We compare our synthetic J-maps with an observed WISPR J-map taken during the fourth solar encounter of PSP and use the observed daily count of tracks in this J-map in conjunction with our synthetic J-maps in order to place constraints on the variability of the solar wind flow properties of slow solar wind transient release in terms of blobs.
We explore the dynamical impacts and observable signatures of
two-fluid effects in the parameter regimes when ion-neutral collisions do not fully couple the neutral and charged fluids.
Popescu Braileanu et al., A&A (2021a,b): doi.org/10.1051/0004-6361/202039053 ; doi.org/10.1051/0004-6361/202140425
We performed 2.5D two-fluid simulations of the Rayleigh-Taylor instability (RTI) at a smoothly
changing interface between a solar prominence thread and the corona.
Our two-fluid model takes into account viscosity, thermal conductivity, and collisional interaction
between neutrals and charges: ionization or recombination, energy and momentum transfer, and frictional heating.
We explore the sensitivity of the RTI dynamics to the prominence equilibrium configuration, including the
impact of the magnetic field strength and shear supporting the prominence thread, the amount of prominence
mass-loading and to collisional effects for different magnetic field configurations supporting the
prominence thread.
At small scales, a realistically smooth prominence-corona interface leads to qualitatively
different linear RTI evolution than that which is expected for a discontinuous interface, while magnetic field shear has
the stabilizing effect of reducing the growth rate or eliminating the instability.
Ionization and recombination reactions
between ionized and neutral fluids do not substantially impact the development of the primary RTI, but they can impact the development of secondary structures during the mixing of the cold prominence
and hotter surrounding coronal material. We find that collisionality within and between ionized and neutral
particle populations plays an important role in both linear and nonlinear development of RTI; ion-neutral
collision frequency is the primary determining factor in development or damping of small-scale structures.
Shocks are regularly observed in the lower solar atmosphere, for example, umbral flashes which have average lifetimes of roughly a minute. For ideal magnetohydrodynamic (MHD) theory, slow-mode shocks should become unstable to the corrugation instability, triggered by the inhomogeneities in the solar atmosphere. However, the lower solar atmosphere is partially ionised, and the presence of a neutral species can stabilise the shock front. Here I present numerical results to investigate the stability conditions for a partially-ionised slow-mode shock with regards to the corrugation instability. Our results indicate that a stability range can be determined based on physical parameters of the system, where partially-ionised shocks are stable depending on the perturbation wavelength relative to the finite shock width. We relate these results to umbral flashes by estimating the wavelengths that could result in a stable shock front, and the observational consequences in terms of observing two-fluid effects in the lower solar atmosphere with the latest instruments.
The Solar X-ray Monitor (XSM) onboard the Chandrayaan-2 mission carries out spectroscopic observations of the Sun in the energy range 1-15 keV with a resolution of 180 eV (at 5.9 keV). Here, we present an overview of results from XSM observation of the Sun during the 2019–2020 solar minimum, considered to be the quietest solar minimum of the past hundred years. These observations provide a unique opportunity to study soft X-ray spectra of the quiescent solar corona and solar transients in absence of major activity. By modeling high-resolution broadband X-ray spectra from XSM, we estimate temperature, emission measure(EM), and absolute abundances of Mg, Al, and Si during periods with no active regions(AR) and very low X-ray intensities, and find a FIP bias of 2, which is lower than the value of 3-4 usually observed in the AR cores. We find that the derived parameters remain nearly constant over time with a temperature around 2 MK, suggesting the emission is dominated by X-ray bright points. During this quiescent period, XSM captured several sub-A class flares that occurred outside conventional ARs. It also observed nine B-class flares ranging from B1.3 to B4.5 originating from isolated ARs. Using time-resolved spectroscopic analysis during these flares, we examine the evolution of temperature, EM, and absolute elemental abundances of four elements- Mg, Al, Si, and S. These are the first measurements of absolute abundances during such small flares. The study offers a unique insight into the evolution of absolute abundances as the flares evolve.
Sunspots consist of a dark umbra and a brighter penumbra. Both regions exhibit magnetoconvection, manifested in penumbral filaments in the penumbra and in umbral dots in the umbra. The origin of the sharp transition from the umbra to the penumbra is unclear.
Here we investigate how the properties of individual convective cells vary across the umbra-penumbra boundary using spectropolarimetric observations of two sunspots performed with the Hinode spacecraft. We compare the physical properties of umbral dots and penumbral filaments by deriving ensemble averages of the physical properties of the different types of convective features.
There are strong similarities between the convective features in the outer parts of the umbra and the ones in the penumbra, with most physical parameters being smooth and continuous functions of the length of the features.
Our results indicate that the transition in brightness from the umbra to the penumbra is solely caused by the larger size and higher brightness of penumbral filaments compared to umbral dots. There is no significant difference in the number density of convective elements between the outer umbra and the inner penumbra. It is still unclear, how exactly the underlying magnetic field causes the increase in size of convective features in the penumbra.
By means of numerical simulations we present a new insight into the propagation of waves in a magnetic arcade embedded in the solar atmosphere and impact of the latter on the observed wave-periods. We consider a 2D approximation of the gravitationally stratified and partially-ionized lower solar atmosphere consisting of ion + electron and neutral fluids that are coupled by ion-neutral collisions. We find that in the solar photosphere, where ions and neutrals are strongly coupled by collisions, magnetoacoustic-gravity and acoustic-gravity waves have periods ranging from 250 s to 350 s. In the chromosphere, where the collisional coupling is weak, the wave characteristics strongly depend on the magnetic field configuration. Above the foot-points of the considered arcade, the plasma is dominated by vertical magnetic field along which ion slow magnetoacoustic-gravity waves are guided. These waves exhibit a broad range of periods with the most prominent periods of 180 s, 220 s, and 300 s. Above the main loop of the solar arcade, where mostly horizontal magnetic field lines guide ion magnetoacoustic waves, the main spectral power reduces to the period of about 180 s and longer wave-periods do not exist. The obtained results demonstrate unprecedented, never reported before level of agreement with the recently reported observational data of Wisniewska et al. (2016) and Kayshap et al. (2018). We demonstrate that the two-fluid approach is indeed crucial for a description of wave-related processes in the lower solar atmosphere, with energy transport and dissipation being of the highest interest among them.
The magnetic reconnection occurs between two magnetic emerging flux (EMF) in a bald patch region observed in HMI vector magnetograms. A transfer of twist was operating between a neighboring flux rope to the jet through the BP.
A spatio-temporal analysis of IRIS spectra of Mg II, C II, and Si IV ions allows us to study the dynamics and the stratification of the flare atmosphere along the line of sight during the magnetic reconnection phase at the jet base in a bald patch region (BP).
The twist was confirmed by tilt of the IRIS spectra well observed in Mg II and Si IV.
Strong asymmetrical Mg II and C II line profiles with extended blue wings observed at the reconnection site are interpreted by the presence of two chromosphere temperature clouds: one explosive cloud with blueshifts at -290 km/s and one cloud with smaller Doppler shift (around -36 km/s). These ejections are in the opposite direction of the jet and explained by trapped cool material between the two EMFs.
The detection of X-ray emission by FERMI/GBM simultaneously with the excess in the Balmer continuum supports the idea of bombardment of non thermal electrons during the reconnection.
There are two types of active region loops in the solar corona: warm loops with temperatures of about 1 MK (Ugarte-Urra et al. 2009) and hot ones with temperatures above 2 MK (Brooks et al. 2008). There are convincing evidence suggesting that the heating mechanism of the "warm loops" is by storms of nanoflares (Warren et al. 2003; Klimchuk 2006, 2009; Ugarte-Urra et al. 2009). However, for "hot coronal loops" there is no agreement on the possible heating mechanism(s). Antichos et al. 2003 using TRACE data concluded that the heating could not be from flare like events, and should be quasi-steady. Some other observations from Hi-C and SDO represented signatures of reconnection events, like coronal nanoflares (Testa et al. 2013). On the other side, there is some observational evidence indicating that magneto-acoustic waves powering the heating in hot coronal loops (Hashim et al. 2021).
High temperatures of hot coronal loops made it hard to resolve the loop structures. Therefore, researchers focused to study the footpoint of hot coronal loops called "moss" to find indirect observational constrains of the existing heating mechanism(s).
In this work using high resolution data of IRIS, along with simultaneous observations of SDO and SOT, and EIS (in HOP 247), we study the moss area properties through spectroscopy and imaging. We found some periodicities in the intensity and linewidth of the C II 1334.5323 emission line in the moss area. More spectral lines are aimed to study in this work to achieve a more solid conclusion.
We investigate abundance variations of heavy ions in coronal loops. We develop and exploit a multi-species model of the solar atmosphere (called IRAP’s Solar Atmospheric Model: ISAM) that solves for the transport of neutral and charged particles from the chromosphere to the corona. We investigate the effect of different mechanisms that could produce the First Ionization Potential (FIP) effect. We compare the effects of the thermal force and of the ponderomotive force. The propagation, reflection and dissipation of Alfvén waves is solved using two distinct models, the first one from Chandran et al. (2011) and the second one that is a more sophisticated turbulence model called Shell-ATM. ISAM solves a set of 16-moment transport equations for both neutrals and charged particles. Protons and heavy ions are heated by Alfvén waves, which then heat up the electrons via collision processes. We show preliminary results on composition distribution along a typical coronal loop and compare with typical FIP biases. This work was funded by the European Research Council through the project SLOW_SOURCE - DLV-819189.
We present our measurements of the tilt of the magnetic-field (MF) axis of sunspots, based on observations of the Sun with microwaves. In contrast to the methods that use the coordinates of the maximum brightness of radio sources located above the sunspots, the new method proposed by us uses measurements of its brightness dynamics. The method is based on a distinctive feature of the cyclotron radiation mechanism - strong suppression of radiation along the MF direction. For an "ideal" (stable, single, and regular) sunspot with a vertical MF, changes in radiation over time should be symmetric with respect to the moment when the sunspot passes through the central meridian of the Sun (PCM) with a minimum brightness at the moment of PCM. The advance or lag of the moment of the minimum relative to the PCM moment can be explained by the inclination of the MF axis to the photosphere surface. Testing of 10 active regions (ARs) of various morphological structures with the RATAN-600 radio telescope and the NoRH radio heliograph showed that in most cases (90%) the axis of the leading sunspot is inclined to the eastern limb and the angle does not depend on the AR morphology. The tilt values at the level of the lower part of the chromosphere – corona transition region are ~ 1–10° and demonstrates an increase with an increase in the height of the radiation source.
Coronal bright points (CBPs) are prominent features of the corona in the quiet-Sun and coronal holes, best observed in extreme-ultraviolet (EUV) and X-ray wavelengths, with lifetimes of up to several hours. They appear as small loops of sizes of about 10-20 Mm connected to bipolar magnetic field concentrations in the photosphere, often associated with flux emergence and cancellation. They can reorganize coronal magnetic fields and often erupt to supply heated material to the upper atmosphere and wind, which makes them important for coronal dynamics.
We report on thermal characteristics of CBPs using first observations from the EUV spectrometer SPICE onboard Solar Orbiter. One unique feature of SPICE is its simultaneous coverage of a broad temperature range from coronal plasma to the low transition region down to 0.01 MK. We utilize this to compare the thermal properties of CBPs with those of the quiet-Sun corona at low temperatures, not accessible to e.g. EIS/Hinode, by conducting differential emission measure (DEM) analysis. Here we can access the minimum of the DEM around log T[K] of ca 5.0 to 5.2 and in particular the gradient of the DEM at lower temperatures towards the chromosphere.
We will present results on how the thermal structure of a CBP differs from the quiet Sun, in particular at low temperatures at the base of the transition region. This should shed new light on where the plasma in a coronal bright point is predominantly heated: from its loop feet or at the top of the brightening loops.
We investigate slow magneto-acoustic waves that are naturally excited by turbulent convection and investigate their role in the energy balance of a plage region using three dimensional (3D) radiation-MHD simulations. We track 25 magnetic field lines both in space and time inside a strong magnetic element and calculate velocity component parallel to the background field and compute the temporal power spectra at various heights above the mean solar surface. Additionally, horizontally averaged power spectra for both longitudinal and vertical components of velocity are calculated using time-series at fixed locations. We also degrade our simulation data to compare our results with observations. The velocity power spectra, averaged horizontally over the whole domain, show that low frequency waves may reach into the chromosphere possibly along the inclined magnetic field lines. In addition, the power spectra at high frequencies follow a power law with an exponent close to -5/3, suggestive of turbulent excitation. The horizontally averaged power spectra of vertical component of velocity at various effective resolutions show that the observed acoustic wave energy fluxes are underestimated, by a factor of three even if determined from observations carried out at a high spatial resolution of 100 km. Since the waves propagate along the non-vertical field lines, measuring the velocity component along the line-of-sight, rather than along the field contributes significantly to this underestimate. Our results show that, in contrast to claims made in the literature, longitudinal waves within magnetic elements carry sufficient energy to heat the chromosphere.
In the near future, the Parker Solar Probe will put theories about the dynamics and nature of the transition between the solar corona and the solar wind to stringent tests. The most popular mechanism aimed to explain the dynamics of the nascent solar wind, including its heating and acceleration, is magnetohydrodynamic (MHD) turbulence. Most of the previous models focused on nonlinear cascade induced by interactions of outgoing Alfvén waves and their reflections, ignoring effects that might be related to perpendicular structuring of the solar coronal plasma,
despite overwhelming evidence for it. In this paper, for the first time, we analyze through 3D MHD numerical simulations the dynamics of the perpendicularly structured solar corona and solar wind, from the low corona to 15 Rs. We find that background structuring has a strong effect on the evolution of MHD turbulence, on much faster timescales than in the perpendicularly homogeneous case. On timescales shorter than nonlinear times, linear effects related to phase mixing result in a 1/f perpendicular energy spectrum. As the turbulent cascade develops, we observe a perpendicular (parallel) energy spectrum with a power-law index of −3/2 or −5/3 (−2), a steeper perpendicular magnetic field than velocity spectrum, and a strong build-up of negative residual energy. We conclude that the turbulence is most probably generated by the self-cascade of the driven transverse kink waves, referred to previously as “uniturbulence,” which might represent the dominant nonlinear energy cascade channel in the pristine solar wind.
Using revised Bent Crystal Spectrometer instrument characteristics, we determined absolute abundances of calcium A(Ca) for 207 flares in their decay phases. The accuracy of abundance determination was the best ever achieved for hot (T > 5 MK) flaring plasma sources, amounting to only 1 - 3 percent for some flares. While the calcium abundance is constant during the decay phase for most cases, for several flares the abundance is observed to change with time. We present patterns of A(Ca) variability for these flares, some of them showing an abundance rise, others a decrease with time during the decay. We discuss the results and present possible physical scenarios which may account for the observed abundance changes.
We present first results of our study to characterize the
dynamics of Alfvén waves in the solar corona. Using MHD
simulations, we study the propagation of
monochromatic Alfvén waves injected at the base of
the corona and quantify their characteristics higher up in
the corona. In particular, we investigate how different flux tube
geometries affect the properties of the waves.
Internal gravity waves are observed in the Earth's atmosphere and oceans, on Mars and Jupiter, and in the Sun's atmosphere. Despite ample evidence for propagating gravity waves in the Sun's atmosphere, we still do not fully understand their characteristics and overall role in the dynamics and energetics of the solar atmosphere. Here we present a new approach to study the propagation of gravity waves in the solar atmosphere, which opens the door for their use in the seismic mapping of the Sun's atmosphere. Our method measures the three-dimensional cross-correlation function between the vertical velocities measured at different heights. We show some preliminary results based on the analysis of both simulations and actual observations, and we outline future developments.
Coronal Mass Ejection (CME) driven shocks are considered to be one of the potential sites to accelerate charged particles. In-situ measurements of CMEs have shown enhancement of particle flux with energies much larger than that of thermal solar wind particles. Nevertheless, understanding such particle energization computationally has been challenging due to the presence of two widely separated scales, where one needs to explore the particles' microphysics along with the macrophysics of the background fluid. In this work, we have examined the probable acceleration mechanisms of such energetic particles using the MHD-PIC approach which is designed to effectively handle the above mentioned scale separation. Our investigation includes simulations of CME-shocks with different Alfvenic Machs along with the variation of the upstream magnetic field's orientation. Particle energy spectrum with a power law slope,f(E)~E$^{-3/2}$, indicates the role of Diffusive Shock Acceleration in parallel shocks. On the other hand, the role of Shock Drift Acceleration is evident for particle energization in quasi-perpendicular shocks. High Mach shocks are found to be better particle accelerators than shocks with low Mach, thereby indicating the role of the shock's strength in the energization process. This work also highlights the presence of different instabilities induced by the escaping high energy particles from the shock front. A combined study of in-situ measurements with such numerical simulations can enrich our understanding of the particle acceleration process in CME-shocks.
Element abundance signatures have long been used as tracers of physical processes throughout astrophysics. Understanding the spatial and temporal variations in the composition of the solar corona provides insight into how matter and energy flow from the solar chromosphere out into the heliosphere. In this work, we investigate the spatial distribution of highly varying plasma composition around one of the largest sunspots of solar cycle 24. Observations of the photosphere, chromosphere, and corona are brought together with magnetic field modeling of the sunspot in order to probe the conditions that regulate the degree of plasma fractionation within loop populations of differing connectivities. Loops above the umbra contain unfractionated plasma, i.e. photospheric composition, while coronal loops rooted in the penumbra contain fractionated plasma with the highest levels observed in the loops that connect within the active region. The distribution of the highly fractionated plasma appears to be correlated with the spatial locations at which intrinsic magnetic perturbations are identified in high spatial resolution spectropolarimetric observations of the solar chromosphere. Tracing field lines from regions of highly fractionated plasma in the corona to locations of magnetic perturbations detected in the chromosphere shows that they are magnetically linked. These results indicate a direct connection between sunspot chromospheric activity and observable changes in coronal plasma composition. We interpret our findings in the wider context of coronal heating and the ponderomotive force model of elemental fractionation.
The beam-plasma interaction plays an important role in solar radio emission. Understanding these mechanisms makes it possible to conclude about the local parameters of the solar plasma and the dynamics of various processes. A powerful, but resource-intensive tool for studying such systems is numerical particle-in-cell simulations. Usually, the infinite plasma approximation is used to describe this system. Its main drawback is the finite margin of the beam nonequilibrium. The beam pumps the wave only until the depth of its potential well in the accompanying reference frame is sufficient to trap beam electrons. After this, the evolution of all waves proceeds in the absence of any energy inflow.
In contrast, in the model with a continuously injected from a local source electron beam, the excited plasma oscillations accumulate at a certain distance from the injection site and form a spatially localized wave packet. The oscillations in this packet are pumped continuously by “fresh” electrons, and their amplitude is saturated at a much higher level than in the temporal problem. Such a model is more resource-intensive, but with the growth of computational power in recent years this has ceased to be a significant problem. In particular, with the help of this model we proposed an interpretation of experiments on radiation generation in plasma with a thin electron beam[1], and also investigated the possibility of a significant increase of the emission level due to a three-wave process in a system with counterstreaming beams[2].
1.Annenkov,V. et al.Phys.Plasmas 26,063104(2019).
2.Annenkov,V. et al.Astrophys.J. 904,88(2020).
Multi-scale vortex motions are ubiquitous in the solar atmosphere. They are already extensively studied by using a number of numerical (magnetohydrostatic and magnetoconvection simulations) and observational (analysis of different spectral lines) approaches. The high-resolution magnetoconvection MuRAM data has been used in this study. For the first time, full 3D photospheric intergranural vortices, defined as coherent structures are substracted from the numerical domain. Lagrangian Averaged Vorticity Deviation (LAVD; Haller,2016, Silva, 2020, 2021) and fluid elements advection were used to identify vortex flows, namely the centre of circulation and their 3D surfaces. The analysis of vortex surfaces was performed by using Proper Orthogonal Decomposition (POD). A number of similarities with hydrodynamic Whirlpool dynamics have been identified. Additionally, the presence of persistent in time surface deformations and possible associated MHD wave propagation will be discussed.
We analyze a C-class solar flare with the microwave (MW) data from Expanded Owens Valley Solar Array (EOVSA) and the SDO/AIA data. We find that the flare is led by an erupting filament. The interesting result is that the flare produces two MW sources, which lay at loop-top region and the region above that, respectively. Moreover, the brightness temperatures of the two sources, as well as derivative curve of GOES soft X-ray flux, change synchronously with a quasi-period of about 40 seconds. At the peak moments, the spectra of both sources show non-thermal gyrosynchrotron characteristics. The results suggest that quasi-periodic magnetic reconnection accelerates electrons, which then produce quasi-periodic MW radiation near the reconnection region and at the loop-top region.
Decayless transverse oscillations of solar coronal loops (or decayless oscillations for short) have attracted great attention since their discovery. Coronal bright points (CBPs) are found to be constituted by small-scale loops. However, the decayless oscillations in CBPs have not been widely reported. In this study, we identified this kind of oscillations in some CBPs using 171 Å images taken by Atmospheric Imaging Assembly (AIA) onboard Solar Dynamics Observatory (SDO). Motion magnification algorithm was used to increase the amplitude, and time-distance diagrams were made to show the oscillatory patterns. We also estimated the loop lengths. Our statistical results show that the average period, displacement amplitude and loop length are about 5 minutes, 0.06 Mm and 22Mm respectively. Moreover, we made a toy model to illustrate how these sub-resolution oscillation amplitudes (less than 0.1 Mm) could be detected. Our study shows that the decayless oscillations also widely exist in small-scale loops of CBPs. And these oscillations might allow for the seismological diagnosing of the quiet-Sun regions.
During solar eruptions, magnetic islands carried by reconnection downflows will encounter second reconnection process when colliding with the loop top. To investigate the second reconnection of magnetic islands, we perform high-resolution 2.5-dimensional MHD simulations of an eruption current sheet (CS) under the high-Lundquist-number and low-$\beta$ coronal environment. The fast reconnection scheme triggered by the plasmoid instability produces various downflow magnetic islands. The rates of the second reconnection of magnetic islands are of the same order as in CS, which also implies that significant magnetic energy can be released on the loop-top region. The intermittent second reconnection of magnetic islands on the loop-top also corresponds to some quasi-periodic characteristics of the solar flare observations. Our results thus imply that the second reconnection of magnetic islands might provide another important mechanism for particle acceleration and loop-top heating, and can explain plenty of small-scale oscillation properties in observations.
Narrow-band bursts (spikes) are very small duration and bandwidth bursts which appear on dynamic spectra from microwave to decametric frequencies; they are believed to be manifestations of small scale energy release through magnetic reconnection. Here we present the results of a study of the characteristics of spike-like structures detected near the front of type-II bursts. We used high sensitivity, low noise dynamic spectra obtained with the acousto-optic analyzer (SAO) of the ARTEMIS-JLS solar radio spectrograph, in conjunction with high time resolution images from the Nançay Radioheliograph (NRH) of a type-II radio burst recorded during the November 3, 2003 extreme solar event. The NRH data provided positional information which were combined with the ARTEMIS-JLS/SAO dynamic spectra. We identified several spikes in the NRH images and measured their size and position. Chains of spike-like structures appear to have a significant contribution to the emission of the type-II burst front. This study indicates that the formation of spike-like chains almost parallel to the type II front are signatures of small-scale reconnection along the shock front. The preponderance of these chains, together with the lack of isolated structures or irregular clusters, points towards some, as yet indeterminate, process inducing some form of order to the reconnection events along the type-II propagating front.
We present the results from the finalized two comprehensive catalogs of solar energetic electron events and their related radio emissions. The solar energetic electron events are detected by the ACE/EPAM instrument covering solar cycles (SC) 23 & 24 in the two energy channels, 103-175 keV and 175-315 keV. The related radio emission signature catalog represents the interplanetary radio emissions related to in situ electrons over two solar cycles, based on space-born and ground-based observatories. The utilized procedure of both catalogs for identifying the electron events, the association to their solar origin and the corresponding radio signatures are described. The statistical relationships between the energetic electrons and their origin (linear and partial correlation analysis) are discussed. The occurrence rates of different radio burst types - II, III or IV - in the interplanetary space related to solar energetic electrons are reported and discussed.
It is well known that not all solar flares are connected with eruptions followed by coronal mass ejection (CME). Even strongest X-class flares may not be accompanied by eruptions or are accompanied by failed eruptions. One of important factor that prevent eruption from developing into CME is strength of the magnetic field overlying flare site. However, few other factors should be considered like solar gravity, filament's internal magnetic tension etc. We present multi-instrument observations of exceptional eruption which was stopped in the LASCO C2 field of view, at the distance of 3 Rʘ from the photosphere. The eruption was observed by SDO\AIA, STEREO A and B, and RHESSI. We performed detailed analysis of eruption's DEM maps, kinematics from three points of view, and HXR emission. Moreover, magnetic fields from PFSS and NLFF models were investigated. This allowed us to analyse in details the energy balance of flare-eruption and episodes of acceleration and deceleration which occurs during the eruption at different heights, leading to stop the eruption eventually.
Solar coronal cavities are dark structures with a rarefied density compared with surrounding streamers. They are often observed as a component of the classic three-part structure of a coronal mass ejections (CME), quiescent cavities are observed mostly in the polar crown regions and may be long-lived. Some of the quiescent cavities may finally erupt as a CME.
We present multi-wavelength observations of previously quiescent cavity during the eruption. Cavity was observed on 15 may 2012. We used SDO/AIA observations to determine Differential Emission Measure (DEM) maps of this structure and studied it's kinematics. We also analysed characteristic lagomorphic structure observed by the Coronal Multichannel Polarimeter (CoMP).
We compared those observations with the forward-modeled emission in EUV and in linear polarisation.
We present four cases of quasi-periodic pulsations (QPPs)
of microwave emission from solar active regions (ARs) on pre-flare phase.
We used the Nobeyama Radioheliograph (NoRH) and
Nobeyama Radio Polarimeters (NoRP) daily observations.
We computed the time series of maximum brightness temperature
and total flux over selected field-of-view (FOV) in three cases and total solar flux in one case.
We found that in all considered cases an increase in the power of QPPs before flares is observed.
The duration of pre-flare wavetrains in periods of oscillations
is approximately the same for all cases and is about 5-10 pulses.
The effect of the occurrence of the QPPs before flares can be interpreted
as a relationship between MHD waves propagating along the magnetic flux tube
of sunspot and beginning of the flares and can be considered as a flare precursor.
The EU Horizon2020 project EUHFORIA 2.0 aims at developing an advanced space weather forecasting tool, combining the MHD solar wind and CME evolution model EUHFORIA[1] with the Solar Energetic Particle (SEP) transport and acceleration model PARADISE[2]. We will first introduce EUHFORIA and PARADISE and then elaborate on the plans of the EUHFORIA 2.0 project which will address the geo-effectiveness of impacts and mitigation to avoid (part of the) damage, including that of extreme events, related to solar eruptions, solar wind streams, and SEPs, with particular emphasis on its application to forecast Geomagnetically Induced Currents (GICs) and radiation on geospace.
The EUHFORIA 2.0 project started on 1 December 2019, and yielded some first results. These concern alternative coronal models, the application of adaptive mesh refinement techniques in the heliospheric part of EUHFORIA, alternative flux-rope CME models, evaluation of data-assimilation based on Karman filtering for the solar wind modelling, and a feasibility study of the integration of SEP models. The novel tool will be accessible by the whole space weather community via the ESA Space Weather Service Network as it will be integrated in the Virtual Space Weather Modelling Centre (VSWMC)[3], which is part of that network.
References
[1]J. Pomoell and S. Poedts: J. of Space Weather and Space Climate, 8, A35 (2018). DOI: https://doi.org/10.1051/swsc/2018020
[2]N. Wijsen, “PARADISE: a model for energetic particle transport in the solar wind”. PhD thesis,April 2020.
[3] S. Poedts, et al.: J. of Space Weather and Space Climate, 10, Art. 14 (2020). Open Access DOI: 10.1051/swsc/2020012
Global magnetic field models use as input synoptic data, which usually show "aging effects" as the 360° information cannot be simultaneously gathered. Most uncertainties come from the far-side which can only be estimated using synoptic charts, surface flux-transport models, or data from helioseismology, however, these are naturally hard to verify.
We present a new method to estimate the far-side open flux from coronal holes using STEREO EUV observations. For this, we correlate the structure of the photospheric magnetic field with features in the transition region. We use properties of the $304$Å intensity distribution specific to coronal holes to derive an empirical estimate for the open flux. Utilizing a large sample of over 300 SDO coronal hole observations we verify this relation. We perform a cross-instrument calibration of the relation to be able to use STEREO data to estimate the open flux at angles not visible from Earth.
We find that the strong, unipolar magnetic elements, that make up most of a coronal holes open flux, can be estimated in the solar transition region as open fields. This is done using the area coverage ($A_{OF}$) of coronal hole structures below a threshold of 78% (STEREO) or 94% (SDO) of the solar disk median intensity as seen in $304$Å filtergrams. From this, it is possible to derive the open magnetic flux of a coronal hole using $|\Phi_{CH}| =A_{CH} * (0.25 \pm 0.06) exp((0.032 ± 0.003)*A_{OF})$ (where $A_{CH}$ is the coronal hole area), with an estimated uncertainty of $40$ to $60\%$.
Large gradual solar energetic particle (SEP) events associated with high-energy protons (up to tens of GeV) can cause hazardous space weather conditions at Earth, pose a severe radiation risk for crewed spaceflight and a significant threat to near-Earth technological assets. We currently do not understand where the SEP seed population originates from and what specific features of a solar active region could be the sources of SEPs. In this study, we investigate the evolution of NOAA active region (AR) 12673, which was the source of four SEP events including one ground level enhancement (GLE 72) in September 2017. We analyse numerous eruptive events from AR 12673, which were either SEP or non-SEP productive, that occurred over a time period of several days between 4-10th September 2017. This is in order to determine what solar precursors, particularly what parameters, configuration and evolution of the magnetic field along with the eruption characteristics are important in SEP-productive source regions and eruptive events. SEP forecasting would hugely benefit from a more advanced understanding of the role of the pre-event source regions and their characteristics.
The 3D MHD modeling is a powerful tool to investigate the physical process responsible for the formation and evolution of the heliosphere and the solar wind. To fully understand the role of each physical ingredient making the model correct, we need a validation process where the output from the simulations are quantitatively compared to the observational data. In this work, we present the results from the validation process for the solar corona of the 3D MHD model WindPredict-AW. We analyze three simulations results, which differ for the initial conditions. We use the density and temperature 3D distributions, output from the simulations for the first Parker Solar Probe perihelion, to synthetize both UV an WL pB images. For these tests, we selected AIA 193 UV emission, MLSO K-Cor and LASCO C2 pB images during 6 and 7 November 2018. We then make quantitative comparisons of the disk and off limb corona. Our tests clearly identify the simulation that provides the best quantitative reproduction of the observed corona, and show that WindPredict-AW is a reliable model.
We study the evolution of the normalized emerging, shearing and total magnetic helicity components for 14 flaring and 14 non-flaring active regions (ARs) using Spaceweather Helioseismic Magnetic Imager Active Region Patches vector magnetic field data (each of the selected AR contains the most complex δ-type spot). Wavelet analysis was performed for each AR. Then we looked for peaks in the periods appearing in the wavelet analysis, after which we performed statistical analyzes. The main findings of this study, (i) the Probability Density Function of peaks found in flaring and non-flaring ARs is that all of distributions of periods appear to be arranged in bands; (ii) from the correlation of the means of Gaussians obtained from Gaussian Mixture Model of ARs we can see that the emerging helicity component clearly becomes separate; (iii) the distributions of peaks before and after the flares changed in the flaring ARs. In all three cases it can be seen that the distribution of periods changes after the flare; (iv) if we see a δ-spot forming but we do not see that the periods in the emerging helicity would be shortened thereby no harmonic properties appear in it, then there is a good probability that flares will not occur; and (v) we can see that long periods (∼20 hour) appear in the total and emerging helicity of flaring ARs, from which it can be concluded that if these periods appear we can expect flares.
The solar radio flux at F10.7 and F30 cm is required by most models characterizing the state of the Earth’s upper atmosphere, such as the thermosphere and ionosphere, to specify satellite orbits, re-entry services, collision avoidance maneuvers, and modeling of the space debris evolution. We develop a method called RESONANCE (Radio Emissions from the Sun: ONline ANalytical Computer-aided Estimator) for the prediction of monthly smoothed F10.7 and F30 indices 1–24 months ahead. The prediction algorithm has three steps. First, we apply a 13-month optimized running mean technique to effectively reduce the noise in the radio flux data. Second, we provide initial predictions of the F10.7 and F30 indices using the McNish–Lincoln method. Finally, we improve these initial predictions by developing an adaptive Kalman filter with error statistics identification. The rms error of predictions with lead times from 1 to 24 months is 5–27 sfu for the F10.7 index and 3–16 sfu for F30, which statistically outperforms current algorithms in use. The proposed approach based on the Kalman filter is universal and can be applied to improve the initial predictions of a process under study provided by any other forecasting method. Furthermore, we present a systematic evaluation of re-entry forecast as an application to test the performance of F10.7 predictions on past ESA re-entry campaigns for payloads, rocket bodies, and space debris that re-entered from 2006 to 2019 June. The test results demonstrate that the predictions obtained by RESONANCE in general also lead to improvements in the forecasts of re-entry epochs.
Inversion techniques are very powerful methods for obtaining information on the thermodynamic and magnetic properties of solar and stellar atmospheres. In recent years, very sophisticated inversion codes have been developed that are now routinely applied to spectro-polarimetric observations. Most of these inversion codes are designed for finding the optimum solution of the nonlinear inverse problem. However, to obtain the location of potentially multimodal cases (ambiguities), the degeneracies, and the uncertainties of each parameter inferred from the inversions, algorithms such as Markov chain Monte Carlo (MCMC) requires to evaluate the likelihood of the model thousand of times and are computationally costly. Variational methods are a quick alternative to Monte Carlo methods by approximating the posterior distribution by a parametrized distribution. In this study, we introduce a highly flexible variational inference method to perform fast Bayesian inference, known as normalizing flows. Normalizing flows are a set of invertible, differentiable, and parametrized transformations that convert a simple distribution into an approximation of any other complex distribution. If the transformations are conditioned on observations, we can train normalizing flows to return Bayesian posterior probability estimates for any observation. We illustrate the ability of the method using a simple Milne-Eddington model and a complex non-LTE inversion. The method is extremely general and other more complex forward models can be applied. The training procedure need only be performed once for a given prior parameter space and the resulting network can then generate samples describing the posterior distribution by several orders of magnitude faster than existing techniques.
Granular lanes are seen in continuum images as features appearing as a bright rim followed by a dark lane traveling into a host granule. With the help of 3-D magnetohydrodynamic simulations it was found that the observed intensity pattern is the visible signature of a subsurface velocity vortex tube. These vortex tubes are regularly generated close to intergranular lanes and have their axis parallel to the solar surface.
We present an analysis of a high-resolution spectropolarimetric data set obtained with the CRISP instrument at the Swedish 1-m Solar Telescope. The data consists of full Stokes measurements in the Fe I 617.3 nm spectral line taken at a cadence of approximately 28 seconds. We detect several cases of granular lanes exhibiting co-spatial elongated linear polarization patches and examine their temporal evolution and magnetic signature. By studying simulations calculated with the CO5BOLD code we are able to investigate the origin of the observed magnetic field. The simulations show several components (lane-aligned, turbulent, or twisted) of magnetic field dominating in different stages of the vortex evolution and revealing a complex magnetic structure. During the process the magnetic field is trapped within the horizontal vortex tube which twists the magnetic fields and transports them into the granules where they emerge to the surface. Our observations therefore are first indications of a “shallow recirculation” process taking place on the Sun.
The magnetically dominated solar corona is structured in the form of loops or flux tubes. To observe this structure during minimum solar activity epochs (or in the quiescent corona) is a difficult task because density and temperature inhomogeneities between loops and their surroundings are relatively low, making them not easily distinguishable in EUV images. Differential emission measure tomography, combined with a global potential model of the coronal magnetic field (DEMT-PFSS), allows us to characterize physical parameters of the coronal plasma along reconstructed loops. In this work, we tomographically reconstruct Carrington Rotation (CR) 2082 that ocurred at the minimum between Solar Cycles 23 and 24 and we statistically analyze the thermodynamic properties of coronal loops. These results are compared with the 1D model, Hydrodynamics and Radiation Code (HYDRAD), for constant and impulsive heating regimes.
The spectral window in the solar photosphere around the magnetically sensitive Cr I lines at 578.2 nm is explored. The goal is to analyze simultaneously 15 spectral lines, which comprise Cr I, Cu I, Fe I, Mn I, and Si I lines, without polarimetry to infer the thermodynamic and magnetic properties in a strongly magnetized plasma using the SIR inversion code.
The study is based on a new detector setup at the Echelle spectrograph of the Vacuum Tower Telescope (VTT) at Tenerife, which enables fast spectroscopic scans. The oscillator strengths of all spectral lines are determined, as well as their response functions to temperature, magnetic field, and Doppler velocity. The snapshot 385 of the Enhanced Network simulation from the Bifrost code serves to synthesize all the lines, which are in turn inverted simultaneously with SIR to establish the best inversion strategy. This strategy is then applied to VTT observations of a sunspot in active region NOAA 12723 on 2018 September 30, and the results are compared to full-disk vector field data obtained with the Helioseismic and Magnetic Imager (HMI).
The analyzed spectral range has the potential to deliver thermal, dynamic, and magnetic information in strongly magnetized features on the Sun, such as pores and sunspots, even without polarimetry. The highest sensitivity of the lines is found in the lower photosphere, on average around optical depth $\log \tau = -1$. The multiple-line inversions provide smooth results across the whole field-of-view.
The Sun has a Near-Surface Shear Layer (NSSL), within which the angular velocity decreases rapidly with radius. We provide an explanation of this layer based on the thermal wind balance equation. Since convective motions are not affected by solar rotation in the top layer of the convection zone, we argue that the temperature falls at the same rate at all latitudes in this layer. This makes the thermal wind term very large in this layer and the centrifugal term has also to become very large to balance it, giving rise to the NSSL. From the values of differential rotation Ω(𝑟 < 𝑟𝑐, 𝜃) at radii less than a radius 𝑟𝑐, we can calculate the temperature difference Δ𝑇 (𝑟, 𝜃) with respect to the standard solar model at different points of the convection zone, by making use of the thermal wind balance equation. Then we again use this equation in the top layer to calculate Ω(𝑟 > 𝑟𝑐, 𝜃) there from Δ𝑇 (𝑟, 𝜃). We carry on this exercise using both an analytical expression of the differential rotation and the actual data provided by helioseismology. We find that our theoretical results of the NSSL match the observational data reasonably well for 𝑟𝑐 ≈ 0.96𝑅⊙, giving an estimate of the radius till which the convective motions are affected by the solar rotation.
High resolution observations of the solar corona with the EUI telescope onboard the Solar Orbiter mission during the perihelion campaign at 0.56 AU revealed omnipresent impulsive quiet-un emissions in the 174 A filter, at previously unresolved temporal/spatial scales. Individual brightenings of the smallest linear size till 0.2Mm show temporal variability within tens of seconds. These EUV quiet sun brightenings, which have been nicknamed campfires, appear as individual quiet-Sun events or simultaneous / consecutive clusters situated along quiescent loops, where usually steadier emission is expected.
The emission measure varies strongly almost in every pixel during the 260 sec observation time. The thermal energy content of individual impulses is calculated from observed emission enhancements and the derived temperature. EUV telescopes indicates heating events observable in coronal iron lines. The observed energy contents vary in the range $10^{21}- 10^{24}$ ergs, which is in agreement with the lower limit estimation of Parker’s nanoflare heating scenario. They occupy a thin vertical layer in the solar corona, as determined by triangulation. The observations suggest that the basic unit of impulsive energy release in EUV corona lies in the range of picoflares, $10^{21}- 10^{24}$ ergs, and may represent a significant part of the missing energy source for coronal heating. Observations were obtained during deep solar minimum, in the absence of any significant flaring activity and active regions.
The article presents a brief overview of the main results of observations of the radio emission of polar coronal holes (CD) on the Sun, obtained in a wide range of wavelengths (m-mm) on various radio telescopes. The results of observations of the polar coronal hole (CD) on RATAN-600 in a wide centimeter wavelength range (1.03-30.7) are analyzed. The obtained physical characteristics of the CD over the North Pole of the Sun are compared with the characteristics of the CD located at lower latitudes.
The solar corona is shaped and mysteriously heated to millions of degrees by the Sun’s magnetic field. It has long been hypothesized that the heating results from a myriad of tiny magnetic energy outbursts called nanoflares, driven by the fundamental process of magnetic reconnection. Misaligned magnetic field lines can break and reconnect, producing nanoflares in avalanche-like processes. However, no direct and unique observations of such nanoflares exist to date, and the lack of a smoking gun has cast doubt on the possibility of solving the coronal heating problem. From coordinated multi-band high-resolution observations, we report on the discovery of very fast and bursty nanojets, the telltale signature of reconnection-based nanoflares resulting in coronal heating. The nanojet is uniquely characterised by being transverse to the loop and appears as a unidirectional jet from the reconnection point. Isolated and clustered nanojets are detected, and a myriad are observed in an avalanche-like progression, leading to the formation of a coronal loop. Using state-of-the-art numerical simulations, we demonstrate that the nanojet is a consequence of the slingshot effect from the magnetically tensed, curved magnetic field lines reconnecting at small angles. Nanojets are therefore the key signature of reconnection-based coronal heating in action.
A quiescent prominence was observed on October 22, 2013 at NW limb quasi-simultaneously and nearly co-spatially in the Lyman line series of hydrogen by SoHO/SUMER and in MgII h&k UV lines by IRIS. In this contribution we analyze a dense and compact structure of the prominence because this part is quiet and therefore suitable for quasi-static non-LTE modeling. This part of the prominence is also well visible in H_alpha filtrogram images. Spectroscopic analysis of the Lyman line and MgII h&k profiles is done using the following profile characteristics: integral intensities, depth of the central reversal and asymmetry of the peaks. Distributions of the profile characteristics within the studied area of the prominence are statistically analyzed using histograms. The profile characteristics are now defined only for profiles with one peak (purely emissive) or double-peaked. There exist also profiles with more peaks in the observed data from both instruments, thus, statistical analysis of occurrences of different type of profiles -- one-, two-, three-, four-and-more-peak profiles and peculiar profiles is also made. Results of the statistical analysis of observed data are to be be compared with the analogous statistical analysis of synthetic profiles obtained using the non-LTE models of the fine structure of prominences.
The interaction between emerging magnetic fields and the preexisting magnetic canopy in active regions is a complex process but essential for understanding the onset of transient brightenings driven by magnetic reconnection and their role in energy/mass deposition in the chromosphere and above.
We present the results of a comprehensive analysis of SST, ALMA, and SDO observations of a solar active region using nonlocal thermodynamic equilibrium inversions, magnetic field extrapolations, and comparisons with 3D radiative magnetohydrodynamics simulations. Inversions of the SST+ALMA dataset constrain the atmospheric stratification and show that enhanced chromospheric temperatures are associated with strong and inclined magnetic fields that connect patches of opposite polarity in the photosphere as revealed by the extrapolation. Simulations show that Ohmic dissipation during flux emergence leads to a range of observational signatures in the millimeter continuum depending on the details of the current sheets from compact, transient brightenings to warm fibril-like structures, both of which have been observed by ALMA.
Waves and oscillatory phenomena have been observed in the solar atmosphere as mechanisms that transfer energy through its different heights, from the photosphere to outer layers. Hence, they are considered as one of the main processes responsible for heating the upper solar atmosphere. This study aims to detect and characterize various MHD wave modes in a sunspot atmosphere (i.e., active region AR12533), based on high-resolution observations with the Swedish 1-m Solar Telescope (SST), complemented by co-observations with the Interface Region Imaging Spectrograph (IRIS) and the Solar Dynamic Observatory (SDO) space missions. The SST observations sample various atmospheric heights in the lower atmosphere, taken in multiple wavelength positions of the Ca II 852.2 nm (in full Stokes) and Hα 656.3 nm spectral line. The MHD waves are traced throughout the solar atmosphere by analysing temporal evolution in intensities and Doppler velocities and shifts in wave frequency. This poster presents the preliminary results and outlines the next steps of these waves propagation analysis.
Observations of fast magnetoacoustic wave trains, also known as quasi-periodic fast-propagating (QFP) waves, at large heights of the Sun’s corona suggest that these waves can travel long distances from the excitation locations. We study characteristic time signatures of fully developed fast magnetoacoustic wave trains guided along the magnetic field by dense plasma slabs in the linear regime. Fast wave trains are excited by a localised impulsive driver and propagate along the waveguide as prescribed by the waveguide-caused dispersion. In slabs with steeper transverse density profiles, developed wave trains are shown to consist of three distinct phases: a long-period quasi-periodic phase with the oscillation period gradually shortening with time, a multi-periodic (peloton) phase in which the harmonics with distinctly different periods co-exist, and a short-lived periodic (Airy) phase. The appearance of these phases is attributed to a non-monotonic dependence of the fast wave group speed on the parallel wavenumber, and is shown to be different for axisymmetric (sausage) and non-axisymmetric (kink) modes. In the Morlet wavelet spectra, this corresponds to the transition from the previously known tadpole-shaped to a boomerang-shaped pattern, with two well-pronounced arms at shorter and longer periods. We describe a specific previously published radio observation of a coronal fast wave train, manifesting the apparent change of the wavelet spectrum shape from a tadpole to a boomerang, which is broadly consistent with our modelling. The applicability of these newly revealed boomerang-shaped fast wave trains for seismological probing of the transverse structuring of the waveguiding coronal plasma is discussed.
The presence of non-Maxwellian distributions in the solar corona is supported by many theoretical calculations and several successful spectroscopic diagnostics from UV and EUV lines in the flares, solar corona and transition region. The kappa-distributions or any other distributions exhibiting high-energy tails can also be expected as a result of particle acceleration processes by nanoflare heating in the solar corona.
Non-Maxwellian distributions generally lead to modification of line intensities compared to Maxwellian ones. This is because rates of individual ionization, recombination and collisional excitation are an integral product of the cross-section multiplied by the distribution. In principle, this enables diagnostics of non-Maxwellian distributions from observed spectra.
The KAPPA software combines our own routines with many modified and original CHIANTI 10 routines and allows comfortable handling like CHIANTI. The extensive KAPPA database contains the total and level resolved excitation, ionization, and recombination rates together with the newest ionization equilibria for kappa-distributions (kappa = 2, 3, 4, 5, 7, 10, 15, 25, and 33). These data together with corresponding atomic data and Maxwellian averaged data are available for all elements and ions included in the CHIANTI. The KAPPA provides fast calculations of synthetic spectra for kappa-distributions, search for diagnostic opportunities, and enables to study the influence of kappa-distributions on the observed temperature distribution in emitting plasma (DEM).
Numerical magnetohydrodynamic (MHD) simulations have become a dominant tool in studies of the non-linear dynamics of solar plasma, such as shock formation, instabilities or magnetic reconnection. Many of the numerical codes used for such simulations have to deal with the stability issues caused by unresolved motions on scales below the grid scale. For that, several algorithms have been developed, i.e. hyper diffusion algorithms, or algorithms based on filtering. Recently, the classical MHD approach is being expanded to treat multiple solar plasma components as independent fluids interacting by collisions. This approach required the numerical scales of fluid interaction to be resolved. In this contribution we study how the numerical diffusion in the explicit two fluid (charges-neutral) Mancha-2F code (Popescu Braileanu et al. 2019a) affects the dynamics of turbulently reconnecting current sheets produced as a results of the non-linear mixing during the Rayleigh-Taylor Instability in a solar prominence. We propose a method to evaluate an equivalent of the Ohmic-like numerical diffusion coefficient, and to estimate the order of dissipation of the numerical scheme.
In the absence of an initial seed, the Biermann battery term of a non-ideal induction equation acts as a source that generates weak magnetic fields. These fields are then amplified via a dynamo mechanism. The Kelvin-Helmholtz instability is a fluid phenomenon that takes place in many astrophysical scenarios and can trigger the action of the Biermann battery and dynamo processes. In this talk, I will present the results from a study in which we investigated the effect that the ionization degree of the plasma and the interaction between the charged and neutral species have on the generation and amplification of these weak magnetic fields. We used the two-fluid model implemented in the numerical code MANCHA-2F to perform 2D simulations. We chose plasma parameters that correspond to the solar chromosphere and a setup with no initial magnetic field and which is unstable due to a velocity shear. We explored a wide range of ionization degrees of the plasma and analyzed the role that the different collisional processes included in the model play on the generation and growth of the magnetic field during the evolution of the Kelvin-Helmholtz instability. We also studied the dependence of the Biermann battery mechanism on the total density of the plasma and the coupling degree between the two fluids. Finally, we performed a comparison of our results with those predicted by a single-fluid model.
Magnetoseismology, a technique of magnetic field diagnostics based on observations of magnetohydrodynamic (MHD) waves, has been widely used to estimate the field strengths of oscillating structures in the solar corona. However, previously magnetoseismology was mostly applied to occasionally occurring oscillation events, providing an estimate of only the average field strength of an oscillating structure, which is usually about 10 Gauss. This restriction could be eliminated if we apply magnetoseismology to the pervasive propagating transverse MHD waves discovered with the Coronal Multi-channel Polarimeter (CoMP). Using several CoMP observations of the Fe XIII 1074.7 nm and 1079.8 nm spectral lines, we obtained maps of the plasma density and wave phase speed in the corona, which allow us to map both the strength and direction of the coronal magnetic field in the plane of sky. We also examined distributions of the electron density and magnetic field strength, and compared their variations with height in the quiet Sun and active regions. Such measurements could provide critical information to advance our understanding of the Sun's magnetism and the magnetic coupling of the whole solar atmosphere.
Waves and oscillations have been shown as a prime means of transporting energy through the solar atmosphere, thus, contributing to the high temperature of the upper layers. In particular, magnetohydrodynamic (MHD) waves are observed in a number of structures in the solar chromosphere, often with observations in the near-ultraviolet (UV) to infrared wavelength range. In this poster, we present our recent work on identification of MHD wave modes in a number of fibrillar structures using high-temporal resolution (i.e., 2~s cadence) observations with the Atacama Large Millimeter/submillimeter Array (ALMA) in Band 6 (centred at 1.2~mm). Such oscillations are further compared with those identified in observations at near- and far-UV wavelengths (i.e., Mg ii k and C ii spectral lines) with the Interface Region Imaging Spectrograph (IRIS) space telescope.
Usually coronal holes (CHs) deviate coronal mass ejections (CMEs) away from them. However, there are some peculiar events reported where the eruption travels towards the CH. To contribute to a space weather forecast efforts, in relation to the prediction of CME trajectories, we study the interaction between flux ropes (FRs) and CHs through numerical simulations. We perform 2.5D numerical simulations where FRs and CHs interact with different relative polarity configurations. The numerical simulations indicate that at low coronal levels, depending on the relative magnetic field polarity between the FR and the CH, the deflection will be attractive, i.e. the FR moves towards the CH (for anti-aligned polarities) or repulsive, i.e. the FR moves away to the CH (for aligned polarities). This is likely due to the formation of vanishing magnetic field regions or null points, located between the FR and the CH or, at the other side of the FR, respectively. We also reconstruct the trajectory and magnetic environment of a peculiar event occurred on 30 April 2012, seen from STEREO spacecrafts.The analysed observational event shows a double-deflection, first departing from the radial direction by approaching the CH and then moving away from it suggesting that the trajectory could result from a magnetic configuration with an anti-aligned polarity. We numerically reproduce the double deflection of the observed event, providing support to this conjecture.
The slowly positively drifting bursts (SPDBs) can occur as a single burst or as a group and its frequency drift is usually less than 300 MHz s^-1. The origin of these burst is unknown and they are observed quite rarely. In our Ondrejov radiospectrograph archive we found up to 10 events during the period 2012-2015 and they are connected with flares. We picked 3 flares for the study. As the radio spectrum does not provide us spatial information, we inspected imaging data from SDO/AIA, in combination with RHESSI and GOES observations to find common features of flares associated with SPDBs.
We investigate the initiation and early evolution of 12 solar eruptions and conclude: (1) The early evolution of all events consists of a slow-rise phase followed by a main-acceleration phase, the height-time profiles of which differ markedly and can be best fit, respectively, by a linear and an exponential function. This indicates that different physical processes dominate in these phases, which is at variance with models that involve a single process. (2) The kinematic evolution of the eruptions tends to be synchronized with the flare light curve in both phases. The synchronization is often but not always close. A delayed onset of the impulsive flare phase is found in the majority of the filament eruptions (five out of six). This delay and its trend to be larger for slower eruptions favor ideal MHD instability models. (3) The average decay index at the onset heights of the main acceleration is close to the threshold of the torus instability for both groups of events, suggesting that this instability initiates and possibly drives the main acceleration.
Geomagnetic storms are the temporary variations of the Earth’s magnetic field, induced by the coronal mass ejection (CME) or the high-speed solar wind stream (HSSWS) with a magnetic field directed oppositely to Earth's. The powerful energy injection into the magnetosphere through the magnetic reconnection during such events directly affects the auroral region of the Earth’s ionosphere, where energetic particles precipitation, auroral oval expansion, and variations of plasma density and field-aligned currents intensity can be observed.
The September 2017’s storm was a strong and complex geomagnetic event during the 24th solar cycle minimum and resulted in dynamic changes in Earth’s magnetosphere-ionosphere-thermosphere (M-I-T) system. The aim of our study is to present an analysis of the relationship between plasma density, solar energetic particles (SEPs), the intensity of field-aligned currents (FACs), and variability of the ionospheric trough position during the geomagnetic storm of 7-8 September 2017. The study is based on Swarm and DMSP satellites data.
We describe turbulent magnetic structure formation via driven magnetic reconnection in the non-linear phase of a Rayleigh-Taylor Instability (RTI) in a solar prominence supported by sheared magnetic field. Solar prominences are formed by partially ionized plasma with inter-particle collision frequencies generally warranting magnetohydrodynamic treatment. In this work, we explore the dynamical impacts and observable signatures of two-fluid effects in the parameter regimes when ion-neutral collisions do not fully couple the neutral and charged fluids [Ref. 1]. We perform 2.5D two-fluid (charges - neutrals) RTI simulations at a smoothly changing interface between a solar prominence thread and the corona. The purpose of this study is to deepen our understanding of the RTI and the effects of the partial ionization on the development of RTI using non-linear two-fluid numerical simulations.
[Ref. 1] Popescu Braileanu et al., A&A (2021a,b): doi.org/10.1051/0004-6361/202039053 ; doi.org/10.1051/0004-6361/202140425
This work was supported by the Spanish Ministry of Science, European Research Council, and the US National Science Foundation. The computations were performed at the Teide High-Performance Computing facilities and LaPalma Supercomputer.
*Any opinion, findings, and conclusions or recommendations expressed in this material are those of the authors and do not necessarily reflect the views of the National Science Foundation.
A key process which leads to eruptive activity in the Sun, is the emergence of the magnetic flux from the solar interior to the solar surface and into the outer solar atmosphere. We present results from 3D numerical simulations, which show the onset of eruptive jets and CME-like structures in emerging flux regions. We discuss the physical connection between jets and large-scale eruptions and the mechanism which drives them.
Direct regular measurements of solar irradiance from space exist since 1978.
They suggest that irradiance varies on all accessible timescales.
Models attributing the variability on time scales longer than about a day to the evolution of the solar surface magnetic field are very successful in reproducing the measured changes.
To reconstruct past irradiance changes, such models require appropriate input data to account for the different contributions of surface magnetic features, such as sunspots and faculae.
Unfortunately, suitable facular data extending before the period of direct irradiance measurements are not available.
Ca II K observations are the longest data that can provide direct information on faculae.
Such data from multiple sources, partly going back to the late 19th century, are an invaluable source of information on past solar activity.
Limiting factors on the use of these data have been the unavailability of the observations in digital form, difficulties in accounting for the non-linear response of the photographic plates to the incident radiation, as well as various artefacts plaguing the images.
We have extensively studied historical Ca II K data, including their photometric calibration and accounting for various large-scale artefacts plaguing them.
We will present our latest work on employment of Ca II K data for reconstructions of past irradiance variations.
Small-scale filament eruptions on the sun have previously been documented in the scientific literature. However, robust techniques to identify and semantically segment them in imagery data have not been developed. In this work, we outline preliminary work in using deep learning algorithms, and convolutional neural networks particularly, to locate mini-filament eruptions. We train a ResNet50 architecture model on H-alpha data, using cross-entropy loss as the criterion for optimization and an Adam optimizer with a learning rate of 0.01. The primary long-
term objective of this work is to find correlations between the occurrences of these eruptions and coronal jets. Automated computer vision methods provide more efficient mechanisms to study long term trends and correlations that would not be possible with conventional methods.
Coronal Mass Ejections (CMEs) are the main drivers of interplanetary shocks and space weather disturbances. One of the key parameters that determine the geo-effectiveness of the CME is its internal magnetic configuration. Strong CMEs directed towards Earth can cause severe damage to our planet. Predicting the arrival time and impact of such CMEs can enable us to mitigate the potential damage to various technological systems on Earth.
Recently, we implemented a novel heliospheric modelin MPI-AMRVAC (Xia et al. (2018)) to improve the predictions of EUHFORIA. Our model solves the ideal MHD equations to obtain a steady state solar wind configuration in a reference frame corotating with the Sun. In addition, CMEs can be modelled by injecting a cone or magnetized CME from the inner boundary (at 0.1 AU). Our implementation in MPI-AMRVAC guarantees efficient performance by using advanced techniques such as radial grid stretching and solution adaptive mesh refinement applied in the inner heliospheric domain.
In this study, we consider the effects of a magnetized CME in the heliosphere. The linear force-free spheromak model from EUHFORIA is injected into the recently-developed heliospheric model in MPI-AMRVAC. We investigate its effect upon interaction with the solar wind. The time series of different variables at L1 are compared to the already-existing spheromak model simulation results in EUHFORIA.
This research has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 870405 (EUHFORIA 2.0).
The slow solar wind and the heliospheric plasma sheet wind is pervaded by periodic density perturbations, which have been identified as the signatures of flux ropes born at the tip of the helmet streamers. In this talk, we propose that the main mechanism controlling this release is a tearing mode. We use MHD simulations of the solar wind and corona to reproduce realistic configurations and outflows surrounding the heliospheric current sheet. The reconnection process, and in particular the fastest growing tearing mode is characterized at various Lundquist numbers in 2D and compared with observations using the ideal tearing scenario. We also study, within 3D simulations, unstable helmet streamer's configurations whose signatures has been measured by Parker Solar Probe and Solar Orbiter during the month of June 2020. These works provide a new fundamental understanding of the inherent variability of the heliospheric plasma sheet, which is essential to reach better forecasting abilities of the Solar-Terrestrial relations.
The near-relativistic electron event of 11th July 2020 was simultaneously observed by Solar Orbiter at a radial distance of 0.61 AU and by the Wind spacecraft at 1 AU. This event exhibited an unusual ratio between the peak intensities recorded by these two spacecraft, which suggests that the coronal transport was substantially suppressed. To model this event we apply our 3d propagation model which includes pitch angle scattering and focused transport. We show that to explain the observed slow decay of electron fluxes at the location of Solar Orbiter one has to consider the existence of a nearby reflecting boundary, which is supported by the magnetic field observations.
This study has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No.\ 101004159 (SERPENTINE).
Solar flares are efficient particle accelerators and prime laboratories for studying astrophysical acceleration and transport processes and our understanding has been enhanced by observationally-driven modelling and multi-wavelength observations from X-rays to (E)UV to radio. During the flare, random motions of the magnetised plasma leading to turbulence may play a vital role in converting magnetic energy to the kinetic energy of accelerated particles. The excess broadening of spectral lines (so-called non-thermal broadening), and in particular spatially resolved (E)UV observations with Hinode/EIS and IRIS, can be used to understand these motions and the important role of turbulence during a flare. Previous studies have shown significant non-thermal broadening in active regions in the pre-flare stages and in flares, although non-thermal broadening generally increases with temperature and height in the coronal loop top source, observations show the presence of non-thermal broadening in all regions of the flare from the loop top source, along loop legs and into the chromosphere. In this talk, I will summarise key observations of solar flare turbulence and discuss the role turbulence plays in solar flare energetic electron acceleration and transport.
Flares and coronal mass ejections (CMEs) cause immediate and adverse effects on the interplanetary space and geospace. In an era of space-based technological civilization, the deeper understanding of the mechanisms that produce them and the construction of efficient prediction schemes are of paramount importance. The source regions of flares and CMEs exhibit some common morphological characteristics, such as $\delta$-spots, filaments and sigmoids, which are associated with strongly sheared magnetic polarity inversion lines, indicative of the complex magnetic configurations that store huge amounts of free magnetic energy and helicity. The challenge is to transform this empirical knowledge into parameters/predictors that can help us distinguish efficiently between quiet, flare-, and CME-productive (eruptive) active regions. Such predictors were first introduced when systematic ground-based observations of the photospheric magnetic field became possible and the relevant research was boosted by the introduction of near real time, uninterrupted, high-quality observations from space, which allowed the study of large, statistically significant samples. Nowadays, machine learning methods accommodate the processing of data of increasing volume and complexity, comprising not only photospheric magnetograms, but also EUV images, spectra, and time series, thus widening our inventory of data sources and feature extraction methods. In this talk I will review these efforts to parameterize the characteristics of eruptive active regions and their application in operational prediction schemes. I will discuss some of the challenges of flare and CME prediction as well as the importance of transforming new knowledge into more efficient predictors and including new types of data.
With the first Solar Orbiter (SO) data being available from the cruise phase, it is now possible to simultaneously observe the Sun from additional vantage points off the Earth-Sun line. One of its instruments, the Polarimetric and Heliospheric Imager (PHI), is the first spectro-polarimeter to operate outside of this line of sight. This opens the opportunity for joint observational campaigns with similar instruments such as the Heliospheric and Magnetic Imager (HMI) on-board the Solar Dynamics Observatory (SDO). We utilise these new observational possibilities to produce combined magnetic synoptic maps from line-of-sight magnetograms of the PHI and HMI instruments. Building on the existing software infrastructure for HMI synoptic maps, we extended its current functionality to include PHI data and correct for the different and varying relative orbital and observational characteristics of the two spacecraft. The results are joint magnetic synoptic maps, that can be produced significantly faster than the approximately 27 days of one solar rotation and therefore are less likely to suffer from the evolution of the magnetic field over the observation period. Once Solar Orbiter leaves the ecliptic plane, we will also plan to include observations of the polar magnetic field into our synoptic maps, which will give an unprecedented insight into the magnetic field of the Sun. In this work, we discuss solutions to the challenges that arise from the substantially different operational environments of the two instruments and give an outlook for the future capabilities of this novel data product.
A solar flare is one of the most impressive solar phenomena emitting a wide range of electromagnetic emission from meter radio to gamma rays. The various mechanisms of radio emission generation allow following all stages of flare evolution from early pre-flare emission to decay phase. Nowadays, modern radio instruments (ALMA, EOVSA, MUSER, LOFAR, SRH, et cetera) provide spectral and spatial information within the range from THz to kHz. These observations allow the solar flare process study from the low chromosphere to interplanetary space. The talk presents the signatures of solar flare radio emission used as the process diagnostic in these phenomena, new achievements and methods that appeared thanks to new modern instruments and discuss the challenges which new observations of radio emission suggested for community discussion.
Solar flares are one of the common sources of solar energetic particles filling the heliosphere. The details of particle acceleration and escape from the solar atmosphere are still a subject of close investigation, and one of the scientific questions addressed by the Solar Orbiter mission. In this paper we will present preliminary results of an event that occurred on 9th May 2021, for which the thermal and non-thermal X-ray signatures were detected both from Solar Orbiter by STIX and from the Earth direction by Fermi/GBM, at different viewing angles. This event was well observed in radio with the ground-based instruments in Nançay: the ORFEES spectrograph and the Nancay Radioheliograph providing both spectral and spatial information . The X-ray event shows both an impulsive phase observed above 25 keV by STIX and FERMI and followed by a more gradual phase observed below 10 keV by STIX. In the decimetric/metric radio domain, this event shows a group of type III bursts extending to the interplanetary medium as well as type IV emission above 400 MHz. We shall discuss here the relative temporal evolutions of HXR emissions at different energies with those of the radio fluxes at different frequencies, as well as the spatial evolution of the radio sources at different frequencies. A first comparison of the HXR spectra of the event viewed under different angles will also been discussed.
In-situ measurements and remote-sensing observations have revealed a rich variety of activities in the solar atmosphere and wind, spanning over a huge amount of time and length scales. In this presentation we will focus on two main basic processes which have an important role in the energetics of the solar wind: (1) the turbulent energy transfer of the electromagnetic and kinetic energy with this correlation to magnetic reconnection processes, (2) and the role of the ambipolar electric field and Coulomb collisions in the acceleration of the solar wind and in shaping the electric velocity distribution functions hence in regulating its heat flux. In this context we will present some results form observations and comparisons with high-resolution fluid and kinetic numerical simulations.
Parker Solar Probe has now completed eight orbits around the Sun, providing a new view of the dynamics of the solar wind in the inner heliosphere all the way down to 14.5 Solar Radii from the surface. This presentation will highlight some important early results, such as the prevalence of Alfvénic turbulence in solar wind of all speeds, the dynamics and evolution of switchbacks, the identification of the sources of the solar wind streams carrying the imprint of coronal structure. A final topic will concern the (in)stability of the forming heliospheric current sheet, and the role of fast reconnecting instabilities in the sources of helmet streamer blobs.
The first encounters of PSP with the Sun revealed the presence of ubiquitous localised magnetic deflections, often called “switchbacks”, in the inner heliosphere. Two main class of theories have emerged in order to explain the formation of these structures: the formation by processes occurring deep in the solar atmosphere or directly in the solar wind. The origin of switchbacks is currently unknown but their omnipresence, however, shows that they could play an important role in the dynamics and heating of the solar wind.
We present the first direct piece of evidence for magnetic reconnection occurring at the boundaries of three switchbacks crossed by PSP at a distance of about 45 radii to the Sun. Analysing the magnetic field and plasma parameters from the FIELDS and SWEAP instruments, we found that these three structures show typical signatures expected for reconnection exhausts at their boundaries. Given the wealth of intense current sheets observed by PSP, reconnection at switchback boundaries appears to be rather rare. However, as the switchback boundaries accommodate currents, one can conjecture that the geometry of these boundaries offers favourable conditions for magnetic reconnection to occur. Such a mechanism would thus contribute in reconfiguring the magnetic field of the switchbacks, affecting the dynamics of the solar wind and eventually contributing to the blending of the structures with the regular wind as they propagate away from the Sun. This is consistent with the current statistical studies showing that there are less switchbacks encountered further away from the Sun.
Space weather previsions require a good balance between speed and accuracy to be able to anticipate the impact of eruptive events at Earth. The strategy used by the european project EUPHORIA 2.0 is to make the best use of various numerical techniques and codes and couple them numerically. This approach however requires a very good description of the corona, as it is the first step of the chain of models that will influence every prevision. Thus it is crucial to be able to provide a coronal model that is both robust, fast and reliable to optimize the chain of previsions.
We have developed a new coronal code based on the COOLFluiD code: having an implicit scheme with adaptative CFL, this allows us to easily optimize the convergence, even for full MHD simulations. As a first step, we have used the polytropic approximation to account for the heating of the corona, before switching to more realistic source terms. We will present here the methods used to benchmark the coronal wind model, using different magnetic configurations and detailed comparisons with other coronal codes. We will then discuss the various numerical optimizations used to accelerate the computation and guarantee an accurate MHD solution within few hours of computation. Finally we will demonstrate the coupling with heliospheric codes to show its forecast abilities.
This project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 870405.
Using combined STEREO‐SOHO white‐light data, we present a method to determine the volume and density of a coronal mass ejection (CME) by applying the graduated cylindrical shell model (GCS) and deprojected mass derivation. Under the assumption that the CME mass is roughly equally distributed within a specific volume, we expand the CME self‐similarly and calculate the CME density for distances close to the Sun (15–30 Rs) and at 1 AU. The procedure is applied on a sample of 29 well‐observed CMEs and compared to their interplanetary counterparts (ICMEs). Specific trends are derived comparing calculated and in‐situ measured proton densities at 1 AU, though large uncertainties are revealed due to the unknown mass and geometry evolution: i) a moderate correlation for the magnetic structure having a mass that stays rather constant (cc ≈ 0.56 − 0.59), and ii) a weak correlation for the sheath density (cc ≈ 0.26) by assuming the sheath region is an extra mass ‐ as expected for a mass pile‐up process ‐ that is in its amount comparable to the initial CME deprojected mass. High correlations are derived between in‐situ measured sheath density and the solar wind density (cc ≈ − 0.73) and solar wind speed (cc ≈ 0.56) as measured 24 hours ahead of the arrival of the disturbance. This confirms that the sheath‐plasma stems from piled‐up solar wind material. While the CME interplanetary propagation speed is not related to the sheath density, the size of the CME may play some role.
After the first discoveries of a different variety of transient phenomena in the solar corona during the 1970s, many recent observations reported that solar coronal jets, which represent an essential manifestation of ubiquitous solar transients, may contribute to the heating of the solar corona and the acceleration of the solar winds. However, the same observations show that jets can be morphologically complex phenomena to study. In this regard, the reconstruction of solar coronal jets in 3D using near-simultaneous observations at different viewpoints allows showing the structure of such events unambiguously.
In the present work, we present the 3D reconstruction of the solar coronal jet that occurred on 2021 February 18 using EUV observations of the Extreme Ultraviolet Imager (EUI) onboard Solar Orbiter (SolO), the Atmospheric Imaging Assembly (AIA) of the Solar Dynamic Observatory (SDO) and the Extreme Ultraviolet Imager (EUVI) onboard STEREO A. Associated with the jet, a GOES A8 class microflare is detected by STIX (Spectrometer/Telescope for Imaging X-rays), the Hard X-ray telescope onboard Solar Orbiter. This unique set of observations provided by three broadly distributed positions in the heliosphere allowed us to apply triangulation techniques, track the evolution of the jet, calculate its kinematics and investigate the flare energy content.
Solar Orbiter got launched in February 2020 into an elliptical orbit around the Sun. Its mission is to perform unprecedented close-up observations of the Sun, provide the first images of the solar polar regions, and investigate the Sun-Earth connection.
The spacecraft carries 10 state-of-the-art instruments composed of Remote Sensing telescopes imaging the Sun in high-resolution and In-Situ sensors measuring the solar wind and magnetic fields in the vicinity of the orbiter.
All instruments were successfully commissioned and then characterised further during the ongoing Cruise Phase. At the end of November 2021, the mission will fly by the Earth for the last time, to reach its initial operational orbit with perihelia as close as 0.28 AU from the Sun, well inside the orbit of Mercury. The spacecraft's unique orbit and the composition of its scientific payload make it very complementary to the existing fleet of solar observatories and heliospheric probes.
On the other hand, both orbit and payload also impose unique constraints on how scientific operations can be conducted. These operations involve long- to very short-term planning in carefully arranged steps, which have much more in common with planetary-encounter missions than preceding heliophysics missions.
In this presentation, we explain the details of how science observations are planned, coordinated and conducted, often very far from Earth, and what plans are made for the first year in the Nominal Mission Phase. We also focus on the high value of coordinated observations with other missions and ground observatories, and how you can get involved.
Magnetic reconnection is a fundamental process for changing the magnetic topology and converting magnetic energy into other forms on the Sun, such as heat, flow energy and fast particle energy. In two dimensions it is fairly well understood, although some aspects still need to be developed. In three dimensions, it behaves very differently and a substantial body of theory and numerical experiment has now been built up, including reconnection at null points, separators and quasi-separators.
Some aspects of solar flares can be understood with 2D reconnection models, but other aspects such as the shapes of flare ribbons, the acceleration of particles and the creation of twist in erupting flux ropes need a 3D understanding. A paradigm shift in our understanding of coronal heating by reconnection has been stimulated by dramatic new observations of photospheric flux cancellation from SUNRISE and from SST together with the realisation that it may well be driving nanoflare heating events and possibly campfires.