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Author name code: valori
ADS astronomy entries on 2022-09-14
author:Valori, Gherardo

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Title: The on-ground data reduction and calibration pipeline for
    SO/PHI-HRT
Authors: Sinjan, J.; Calchetti, D.; Hirzberger, J.; Orozco Suárez,
   D.; Albert, K.; Albelo Jorge, N.; Appourchaux, T.; Alvarez-Herrero,
   A.; Blanco Rodríguez, J.; Gandorfer, A.; Germerott, D.; Guerrero,
   L.; Gutierrez Marquez, P.; Kahil, F.; Kolleck, M.; Solanki, S. K.; del
   Toro Iniesta, J. C.; Volkmer, R.; Woch, J.; Fiethe, B.; Gómez Cama,
   J. M.; Pérez-Grande, I.; Sanchis Kilders, E.; Balaguer Jiménez,
   M.; Bellot Rubio, L. R.; Carmona, M.; Deutsch, W.; Fernandez-Rico,
   G.; Fernández-Medina, A.; García Parejo, P.; Gasent Blesa, J. L.;
   Gizon, L.; Grauf, B.; Heerlein, K.; Korpi-Lagg, A.; Lange, T.; López
   Jiménez, A.; Maue, T.; Meller, R.; Michalik, H.; Moreno Vacas, A.;
   Müller, R.; Nakai, E.; Schmidt, W.; Schou, J.; Schühle, U.; Staub,
   J.; Strecker, H.; Torralbo, I.; Valori, G.
2022arXiv220814904S    Altcode:
  The ESA/NASA Solar Orbiter space mission has been successfully launched
  in February 2020. Onboard is the Polarimetric and Helioseismic Imager
  (SO/PHI), which has two telescopes, a High Resolution Telescope
  (HRT) and the Full Disc Telescope (FDT). The instrument is designed
  to infer the photospheric magnetic field and line-of-sight velocity
  through differential imaging of the polarised light emitted by the
  Sun. It calculates the full Stokes vector at 6 wavelength positions
  at the Fe I 617.3 nm absorption line. Due to telemetry constraints,
  the instrument nominally processes these Stokes profiles onboard,
  however when telemetry is available, the raw images are downlinked and
  reduced on ground. Here the architecture of the on-ground pipeline
  for HRT is presented, which also offers additional corrections not
  currently available on board the instrument. The pipeline can reduce
  raw images to the full Stokes vector with a polarimetric sensitivity
  of $10^{-3}\cdot I_{c}$ or better.

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Title: Investigating of the nature of magnetic oscillations associated
    with FIP effect
Authors: Murabito, Mariarita; Jafarzadeh, Shahin; Van Driel-Gesztelyi,
   Lidia; Ermolli, Ilaria; Baker, Deborah; Brooks, David; Long, David;
   Jess, David; Valori, Gherardo; Stangalini, Marco
2022cosp...44.2591M    Altcode:
  Observations of the photosphere, chromosphere, and corona combined with
  magnetic field modeling of one of the biggest sunspots of the 24 solar
  cycle, revealed that regions of high FIP bias plasma in the corona
  were magnetically linked to the locations of the intrinsic magnetic
  oscillations in the solar chromosphere. In order to characterize
  the driver of the oscillations, we analyzed the relation between
  the spatial distribution of the magnetic wave power and the overall
  field geometry and plasma parameters obtained from the multi-height
  spectropolarimetric non-local thermodynamic equilibrium (NLTE)
  inversions. In correspondence with the locations where the magnetic
  wave energy is observed at chromospheric heights, we found evidence
  in support of locally excited acoustic waves that, after crossing the
  equipartition layer located close to the umbra-penumbra boundary at
  photospheric heights, are converted into magnetic-like waves. These
  results indicate a direct connection between sunspot chromospheric
  activity and observable changes in coronal plasma composition,
  demonstrating the power of high resolution, multi-height studies of the
  solar atmosphere that will become the gold standard in the era of DKIST.

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Title: Understanding the Correlation between Solar Coronal Abundances
    and F10.7 Radio Emission
Authors: To, Andy S. H.; Baker, Deborah; Long, David; James, Alexander;
   Brooks, David; van Driel-Gesztelyi, Lidia; Valori, Gherardo; Bastian,
   Tim; Lomuscio, Samantha; Stansby, David
2022cosp...44.2592T    Altcode:
  Solar corona plasma composition, derived from full-Sun spectra, and
  the F10.7 radio flux (2.8 GHz) have been shown to be highly correlated
  (r = 0.88) during the recent weak solar cycle. However, this correlation
  becomes nonlinear at times of increased solar magnetic activity. We used
  co-temporal, high spatial resolution, radio (JVLA), and EUV (Hinode/EIS)
  images of the Sun taken on the 3 and 7 April 2020 to understand the
  underlying causes of the non-linearity of the FIP bias-F10.7 solar
  index correlation. We then calculated differential emission measures
  from AIA images, and paired them with the observed FIP bias to predict
  the bremsstrahlung component of F10.7 radio emission. Results of this
  study provide constraints on the amplitude of composition variability
  related to solar cycle amplitude, and provide an alternative method
  to calculate coronal composition.

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Title: Evolution of Plasma Composition in an Eruptive Flux Rope
Authors: Baker, Deborah; Demoulin, Pascal; Long, David; Janvier, Miho;
   Green, Lucie; Brooks, David; van Driel-Gesztelyi, Lidia; Mihailescu,
   Teodora; To, Andy S. H.; Yardley, Stephanie; Valori, Gherardo
2022cosp...44.1361B    Altcode:
  Magnetic flux ropes are bundles of twisted magnetic field enveloping a
  central axis. They harbor free magnetic energy and can be progenitors
  of coronal mass ejections (CMEs). However, identifying flux ropes on
  the Sun can be challenging. One of the key coronal observables that
  has been shown to indicate the presence of a flux rope is a peculiar
  bright coronal structure called a sigmoid. In this work, we show Hinode
  EUV Imaging Spectrometer observations of sigmoidal active region (AR)
  10977. We analyze the coronal plasma composition in the AR and its
  evolution as a sigmoid (flux rope) forms and erupts as a CME. Plasma
  with photospheric composition was observed in coronal loops close to
  the main polarity inversion line during episodes of significant flux
  cancellation, suggestive of the injection of photospheric plasma into
  these loops driven by photospheric flux cancellation. Concurrently,
  the increasingly sheared core field contained plasma with coronal
  composition. As flux cancellation decreased and a sigmoid/flux
  rope formed, the plasma evolved to an intermediate composition in
  between photospheric and typical AR coronal compositions. Finally,
  the flux rope contained predominantly photospheric plasma during and
  after a failed eruption preceding the CME. Hence, plasma composition
  observations of AR 10977 strongly support models of flux rope formation
  by photospheric flux cancellation forcing magnetic reconnection first
  at the photospheric level then at the coronal level.

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Title: The identification of magnetic perturbations in the solar
    atmosphere
Authors: Stangalini, Marco; Jafarzadeh, Shahin; Baker, Deborah; Jess,
   David; Murabito, Mariarita; Valori, Gherardo
2022cosp...44.2590S    Altcode:
  Magneto-hydrodynamic (MHD) waves and, in particular, magnetic
  perturbations associated with specific wave modes are thought to be
  important mechanisms not only for the heating of the outer layers of
  the Sun's atmosphere, but also for the elemental abundance anomaly
  observed in the corona. High resolution spectropolarimetry is nowadays
  progressively extending to the upper layers of the solar atmosphere,
  and this provides invaluable insight into MHD wave processes up to
  chromospheric heights. However, the identification of real magnetic
  perturbations remains a difficult task due to a number of spurious
  effects that can mimic the signals associated with them. In this
  contribution we will show a novel approach to the identification
  of real magnetic oscillations potentially linked to FIP and discuss
  proxies to be used in statistical analyses.

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Title: The magnetic drivers of campfires seen by the Polarimetric
    and Helioseismic Imager (PHI) on Solar Orbiter
Authors: Kahil, F.; Hirzberger, J.; Solanki, S. K.; Chitta, L. P.;
   Peter, H.; Auchère, F.; Sinjan, J.; Orozco Suárez, D.; Albert,
   K.; Albelo Jorge, N.; Appourchaux, T.; Alvarez-Herrero, A.; Blanco
   Rodríguez, J.; Gandorfer, A.; Germerott, D.; Guerrero, L.; Gutiérrez
   Márquez, P.; Kolleck, M.; del Toro Iniesta, J. C.; Volkmer, R.;
   Woch, J.; Fiethe, B.; Gómez Cama, J. M.; Pérez-Grande, I.; Sanchis
   Kilders, E.; Balaguer Jiménez, M.; Bellot Rubio, L. R.; Calchetti,
   D.; Carmona, M.; Deutsch, W.; Fernández-Rico, G.; Fernández-Medina,
   A.; García Parejo, P.; Gasent-Blesa, J. L.; Gizon, L.; Grauf, B.;
   Heerlein, K.; Lagg, A.; Lange, T.; López Jiménez, A.; Maue, T.;
   Meller, R.; Michalik, H.; Moreno Vacas, A.; Müller, R.; Nakai,
   E.; Schmidt, W.; Schou, J.; Schühle, U.; Staub, J.; Strecker, H.;
   Torralbo, I.; Valori, G.; Aznar Cuadrado, R.; Teriaca, L.; Berghmans,
   D.; Verbeeck, C.; Kraaikamp, E.; Gissot, S.
2022A&A...660A.143K    Altcode: 2022arXiv220213859K
  Context. The Extreme Ultraviolet Imager (EUI) on board the Solar Orbiter
  (SO) spacecraft observed small extreme ultraviolet (EUV) bursts,
  termed campfires, that have been proposed to be brightenings near the
  apexes of low-lying loops in the quiet-Sun atmosphere. The underlying
  magnetic processes driving these campfires are not understood. <BR
  /> Aims: During the cruise phase of SO and at a distance of 0.523
  AU from the Sun, the Polarimetric and Helioseismic Imager on Solar
  Orbiter (SO/PHI) observed a quiet-Sun region jointly with SO/EUI,
  offering the possibility to investigate the surface magnetic field
  dynamics underlying campfires at a spatial resolution of about 380
  km. <BR /> Methods: We used co-spatial and co-temporal data of the
  quiet-Sun network at disc centre acquired with the High Resolution
  Imager of SO/EUI at 17.4 nm (HRI<SUB>EUV</SUB>, cadence 2 s) and the
  High Resolution Telescope of SO/PHI at 617.3 nm (HRT, cadence 2.5
  min). Campfires that are within the SO/PHI−SO/EUI common field
  of view were isolated and categorised according to the underlying
  magnetic activity. <BR /> Results: In 71% of the 38 isolated events,
  campfires are confined between bipolar magnetic features, which seem to
  exhibit signatures of magnetic flux cancellation. The flux cancellation
  occurs either between the two main footpoints, or between one of the
  footpoints of the loop housing the campfire and a nearby opposite
  polarity patch. In one particularly clear-cut case, we detected the
  emergence of a small-scale magnetic loop in the internetwork followed
  soon afterwards by a campfire brightening adjacent to the location
  of the linear polarisation signal in the photosphere, that is to
  say near where the apex of the emerging loop lays. The rest of the
  events were observed over small scattered magnetic features, which
  could not be identified as magnetic footpoints of the campfire hosting
  loops. <BR /> Conclusions: The majority of campfires could be driven
  by magnetic reconnection triggered at the footpoints, similar to the
  physical processes occurring in the burst-like EUV events discussed
  in the literature. About a quarter of all analysed campfires, however,
  are not associated to such magnetic activity in the photosphere, which
  implies that other heating mechanisms are energising these small-scale
  EUV brightenings.

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Title: Evolution of Plasma Composition in an Eruptive Flux Rope
Authors: Baker, D.; Green, L. M.; Brooks, D. H.; Démoulin, P.;
   van Driel-Gesztelyi, L.; Mihailescu, T.; To, A. S. H.; Long, D. M.;
   Yardley, S. L.; Janvier, M.; Valori, G.
2022ApJ...924...17B    Altcode: 2021arXiv211011714B
  Magnetic flux ropes are bundles of twisted magnetic field enveloping a
  central axis. They harbor free magnetic energy and can be progenitors
  of coronal mass ejections (CMEs). However, identifying flux ropes on
  the Sun can be challenging. One of the key coronal observables that
  has been shown to indicate the presence of a flux rope is a peculiar
  bright coronal structure called a sigmoid. In this work, we show Hinode
  EUV Imaging Spectrometer observations of sigmoidal active region (AR)
  10977. We analyze the coronal plasma composition in the AR and its
  evolution as a sigmoid (flux rope) forms and erupts as a CME. Plasma
  with photospheric composition was observed in coronal loops close to
  the main polarity inversion line during episodes of significant flux
  cancellation, suggestive of the injection of photospheric plasma into
  these loops driven by photospheric flux cancellation. Concurrently,
  the increasingly sheared core field contained plasma with coronal
  composition. As flux cancellation decreased and a sigmoid/flux
  rope formed, the plasma evolved to an intermediate composition in
  between photospheric and typical AR coronal compositions. Finally,
  the flux rope contained predominantly photospheric plasma during and
  after a failed eruption preceding the CME. Hence, plasma composition
  observations of AR 10977 strongly support models of flux rope formation
  by photospheric flux cancellation forcing magnetic reconnection first
  at the photospheric level then at the coronal level.

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Title: Disambiguation of Vector Magnetograms by Stereoscopic
    Observations from the Solar Orbiter (SO)/Polarimetric and Helioseismic
    Imager (PHI) and the Solar Dynamic Observatory (SDO)/Helioseismic
    and Magnetic Imager (HMI)
Authors: Valori, Gherardo; Löschl, Philipp; Stansby, David; Pariat,
   Etienne; Hirzberger, Johann; Chen, Feng
2022SoPh..297...12V    Altcode: 2021arXiv211210650V
  Spectropolarimetric reconstructions of the photospheric vector magnetic
  field are intrinsically limited by the 180<SUP>∘</SUP> ambiguity
  in the orientation of the transverse component. The successful
  launch and operation of Solar Orbiter have made the removal of
  the 180<SUP>∘</SUP> 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 spacecrafts' orbits and
  measurement principles. In this work, we present a stereoscopic
  disambiguation method (SDM) and discuss thorough testing of its
  accuracy in applications to modeled active regions and quiet-Sun
  observations. In the first series of tests, we employ magnetograms
  extracted from three different numerical simulations as test fields
  and model observations of the magnetograms from different angles and
  distances. In these more idealized tests, SDM is proven to reach a 100%
  disambiguation accuracy when applied to moderately-to-well resolved
  fields. In such favorable conditions, the accuracy is almost independent
  of the relative position of the spacecraft with the obvious exceptions
  of configurations where the spacecraft are within a few degrees of
  co-alignment or quadrature. Even in the case of disambiguation of
  quiet-Sun magnetograms with significant under-resolved spatial scales,
  SDM provides an accuracy between 82% and 98%, depending on the field
  strength. The accuracy of SDM is found to be mostly sensitive to the
  variable spatial resolution of Solar Orbiter in its highly elliptic
  orbit, as well as to the intrinsic spatial scale of the observed
  field. Additionally, we provide an example of the expected accuracy as
  a function of time that can be used to optimally place remote-sensing
  observing windows during Solar Orbiter observation planning. Finally,
  as a more realistic test, we consider magnetograms that are obtained
  using a radiative-transfer inversion code and the SO/PHI Software
  siMulator (SOPHISM) applied to a 3D-simulation of a pore, and we
  present a preliminary discussion of the effect of the viewing angle
  on the observed field. In this more realistic test of the application
  of SDM, the method is able to successfully remove the ambiguity in
  strong-field areas.

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Title: Investigating the origin of magnetic perturbations associated
    with the FIP Effect
Authors: Murabito, M.; Stangalini, M.; Baker, D.; Valori, G.; Jess,
   D. B.; Jafarzadeh, S.; Brooks, D. H.; Ermolli, I.; Giorgi, F.; Grant,
   S. D. T.; Long, D. M.; van Driel-Gesztelyi, L.
2021A&A...656A..87M    Altcode: 2021arXiv210811164M
  Recently, magnetic oscillations were detected in the chromosphere
  of a large sunspot and found to be linked to the coronal locations
  where a first ionization potential (FIP) effect was observed. In
  an attempt to shed light on the possible excitation mechanisms
  of these localized waves, we further investigate the same data
  by focusing on the relation between the spatial distribution of
  the magnetic wave power and the overall field geometry and plasma
  parameters obtained from multi-height spectropolarimetric non-local
  thermodynamic equilibrium (NLTE) inversions of IBIS data. We find,
  in correspondence with the locations where the magnetic wave energy
  is observed at chromospheric heights, that the magnetic fields have
  smaller scale heights, meaning faster expansions of the field lines,
  which ultimately results in stronger vertical density stratification
  and wave steepening. In addition, the acoustic spectrum of the
  oscillations at the locations where magnetic perturbations are
  observed is broader than that observed at other locations, which
  suggests an additional forcing driver to the p-modes. Analysis of the
  photospheric oscillations in the sunspot surroundings also reveals
  a broader spectrum between the two opposite polarities of the active
  region (the leading spot and the trailing opposite polarity plage),
  and on the same side where magnetic perturbations are observed in
  the umbra. We suggest that strong photospheric perturbations between
  the two polarities are responsible for this broader spectrum of
  oscillations, with respect to the p-mode spectrum, resulting in locally
  excited acoustic waves that, after crossing the equipartition layer,
  located close to the umbra-penumbra boundary at photopheric heights,
  are converted into magnetic waves and steepen due to the strong
  density gradient. <P />Movie associated to Fig. 1 is available at <A
  href="https://www.aanda.org/10.1051/0004-6361/202141504/olm">https://www.aanda.org</A>

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Title: Localized Acceleration of Energetic Particles by a Weak Shock
    in the Solar Corona
Authors: Long, David M.; Reid, Hamish A. S.; Valori, Gherardo;
   O'Kane, Jennifer
2021ApJ...921...61L    Altcode: 2021arXiv210805068L
  Globally propagating shocks in the solar corona have long been studied
  to quantify their involvement in the acceleration of energetic
  particles. However, this work has tended to focus on large events
  associated with strong solar flares and fast coronal mass ejections
  (CMEs), where the waves are sufficiently fast to easily accelerate
  particles to high energies. Here we present observations of particle
  acceleration associated with a global wave event which occurred on
  2011 October 1. Using differential emission measure analysis, the
  global shock wave was found to be incredibly weak, with an Alfvén
  Mach number of ~1.008-1.013. Despite this, spatially resolved type III
  radio emission was observed by the Nançay RadioHeliograph at distinct
  locations near the shock front, suggesting localized acceleration
  of energetic electrons. Further investigation using magnetic field
  extrapolation identified a fan structure beneath a magnetic null located
  above the source active region, with the erupting CME contained within
  this topological feature. We propose that a reconfiguration of the
  coronal magnetic field driven by the erupting CME enabled the weak
  shock to accelerate particles along field lines initially contained
  within the fan and subsequently opening into the heliosphere, producing
  the observed type III emission. These results suggest that even weak
  global shocks in the solar corona can accelerate energetic particles
  via reconfiguration of the surrounding magnetic field.

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Title: Magnetic Helicity Estimations in Models and Observations of
    the Solar Magnetic Field. IV. Application to Solar Observations
Authors: Thalmann, J. K.; Georgoulis, M. K.; Liu, Y.; Pariat, E.;
   Valori, G.; Anfinogentov, S.; Chen, F.; Guo, Y.; Moraitis, K.; Yang,
   S.; Mastrano, Alpha; ISSI Team on Magnetic Helicity
2021ApJ...922...41T    Altcode: 2021arXiv210808525T
  In this ISSI-supported series of studies on magnetic helicity in the
  Sun, we systematically implement 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 data from Hinode's Solar Optical
  Telescope. The target is NOAA Active Region 10930 during a 1.5-day
  interval in 2006 December that included a major eruptive flare
  (SOL2006-12-13T02:14X3.4). Finite-volume and connectivity-based methods
  yield instantaneous budgets of the coronal magnetic helicity, while
  the flux-integration methods allow an estimate of the accumulated
  helicity injected through the photosphere. 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, (iii) an excellent agreement between the flux-integration
  methods, and (iv) an overall agreement between finite-volume- and
  flux-integration-based estimates regarding the predominant sign and
  magnitude of the helicity. To the second objective, we are confident
  that the photospheric helicity flux significantly contributed to the
  coronal helicity budget and that a right-handed structure erupted from
  a predominantly left-handed corona during the X-class flare. Overall,
  we find that the use of different methods to estimate the (accumulated)
  coronal helicity may be necessary in order to draw a complete picture
  of an active region corona, given the careful handling of identified
  data (preparation) issues, which otherwise would mislead the event
  analysis and interpretation.

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Title: Plasma Upflows Induced by Magnetic Reconnection Above an
    Eruptive Flux Rope
Authors: Baker, Deborah; Mihailescu, Teodora; Démoulin, Pascal;
   Green, Lucie M.; van Driel-Gesztelyi, Lidia; Valori, Gherardo; Brooks,
   David H.; Long, David M.; Janvier, Miho
2021SoPh..296..103B    Altcode: 2021arXiv210616137B
  One of the major discoveries of Hinode's Extreme-ultraviolet
  Imaging Spectrometer (EIS) is the presence of upflows at the edges
  of active regions. As active regions are magnetically connected
  to the large-scale field of the corona, these upflows are a likely
  contributor to the global mass cycle in the corona. Here we examine
  the driving mechanism(s) of the very strong upflows with velocities
  in excess of 70 km s<SUP>−1</SUP>, known as blue-wing asymmetries,
  observed during the eruption of a flux rope in AR 10977 (eruptive flare
  SOL2007-12-07T04:50). We use Hinode/EIS spectroscopic observations
  combined with magnetic-field modeling to investigate the possible
  link between the magnetic topology of the active region and the strong
  upflows. A Potential Field Source Surface (PFSS) extrapolation of the
  large-scale field shows a quadrupolar configuration with a separator
  lying above the flux rope. Field lines formed by induced reconnection
  along the separator before and during the flux-rope eruption are
  spatially linked to the strongest blue-wing asymmetries in the upflow
  regions. The flows are driven by the pressure gradient created when
  the dense and hot arcade loops of the active region reconnect with
  the extended and tenuous loops overlying it. In view of the fact
  that separator reconnection is a specific form of the more general
  quasi-separatrix (QSL) reconnection, we conclude that the mechanism
  driving the strongest upflows is, in fact, the same as the one driving
  the persistent upflows of ≈10 - 20 km s<SUP>−1</SUP> observed in
  all active regions.

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Title: The Evolution of Plasma Composition during a Solar Flare
Authors: To, Andy S. H.; Long, David M.; Baker, Deborah; Brooks, David
   H.; van Driel-Gesztelyi, Lidia; Laming, J. Martin; Valori, Gherardo
2021ApJ...911...86T    Altcode: 2021arXiv210209985T
  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 &lt;
  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.

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Title: Matching Temporal Signatures of Solar Features to Their
    Corresponding Solar-Wind Outflows
Authors: de Pablos, D.; Long, D. M.; Owen, C. J.; Valori, G.; Nicolaou,
   G.; Harra, L. K.
2021SoPh..296...68D    Altcode: 2021arXiv210309077D
  The role of small-scale coronal eruptive phenomena in the generation
  and heating of the solar wind remains an open question. Here, we
  investigate the role played by coronal jets in forming the solar wind
  by testing whether temporal variations associated with jetting in EUV
  intensity can be identified in the outflowing solar-wind plasma. This
  type of comparison is challenging due to inherent differences between
  remote-sensing observations of the source and in-situ observations
  of the outflowing plasma, as well as travel time and evolution
  of the solar wind throughout the heliosphere. To overcome these,
  we propose a novel algorithm combining signal filtering, two-step
  solar-wind ballistic back-mapping, window shifting, and Empirical
  Mode Decomposition. We first validate the method using synthetic data,
  before applying it to measurements from the Solar Dynamics Observatory
  and Wind spacecraft. The algorithm enables the direct comparison of
  remote-sensing observations of eruptive phenomena in the corona to
  in-situ measurements of solar-wind parameters, among other potential
  uses. After application to these datasets, we find several time windows
  where signatures of dynamics found in the corona are embedded in
  the solar-wind stream, at a time significantly earlier than expected
  from simple ballistic back-mapping, with the best-performing in-situ
  parameter being the solar-wind mass flux.

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Title: Spectropolarimetric fluctuations in a sunspot chromosphere
Authors: Stangalini, M.; Baker, D.; Valori, G.; Jess, D. B.;
   Jafarzadeh, S.; Murabito, M.; To, A. S. H.; Brooks, D. H.; Ermolli,
   I.; Giorgi, F.; MacBride, C. D.
2021RSPTA.37900216S    Altcode: 2020arXiv200905302S
  The instrumental advances made in this new era of 4 m class solar
  telescopes with unmatched spectropolarimetric accuracy and sensitivity
  will enable the study of chromospheric magnetic fields and their
  dynamics with unprecedented detail. In this regard, spectropolarimetric
  diagnostics can provide invaluable insight into magneto-hydrodynamic
  (MHD) wave processes. MHD waves and, in particular, Alfvénic
  fluctuations associated with particular wave modes were recently
  recognized as important mechanisms not only for the heating of the outer
  layers of the Sun's atmosphere and the acceleration of the solar wind,
  but also for the elemental abundance anomaly observed in the corona
  of the Sun and other Sun-like stars (also known as first ionization
  potential) effect. Here, we take advantage of state-of-the-art and
  unique spectropolarimetric Interferometric BIdimensional Spectrometer
  observations to investigate the relation between intensity and circular
  polarization (CP) fluctuations in a sunspot chromosphere. Our results
  show a clear link between the intensity and CP fluctuations in a patch
  which corresponds to a narrow range of magnetic field inclinations. This
  suggests the presence of Alfvénic perturbations in the sunspot. <P
  />This article is part of the Theo Murphy meeting issue `High-resolution
  wave dynamics in the lower solar atmosphere'.

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Title: The Magnetic Environment of a Stealth Coronal Mass Ejection
Authors: O'Kane, Jennifer; Mac Cormack, Cecilia; Mandrini, Cristina H.;
   Démoulin, Pascal; Green, Lucie M.; Long, David M.; Valori, Gherardo
2021ApJ...908...89O    Altcode: 2020arXiv201203757O
  Interest in stealth coronal mass ejections (CMEs) is increasing due to
  their relatively high occurrence rate and space weather impact. However,
  typical CME signatures such as extreme-ultraviolet dimmings and
  post-eruptive arcades are hard to identify and require extensive image
  processing techniques. These weak observational signatures mean that
  little is currently understood about the physics of these events. We
  present an extensive study of the magnetic field configuration in which
  the stealth CME of 2011 March 3 occurred. Three distinct episodes
  of flare ribbon formation are observed in the stealth CME source
  active region (AR). Two occurred prior to the eruption and suggest the
  occurrence of magnetic reconnection that builds the structure that will
  become eruptive. The third occurs in a time close to the eruption of
  a cavity that is observed in STEREO-B 171 Å data; this subsequently
  becomes part of the propagating CME observed in coronagraph data. We
  use both local (Cartesian) and global (spherical) models of the coronal
  magnetic field, which are complemented and verified by the observational
  analysis. We find evidence of a coronal null point, with field lines
  computed from its neighborhood connecting the stealth CME source region
  to two ARs in the northern hemisphere. We conclude that reconnection
  at the null point aids the eruption of the stealth CME by removing the
  field that acted to stabilize the preeruptive structure. This stealth
  CME, despite its weak signatures, has the main characteristics of
  other CMEs, and its eruption is driven by similar mechanisms.

---------------------------------------------------------
Title: Flaring activity and related eruptions from active regions
Authors: Green, Lucie; Long, David; Valori, Gherardo; O'Kane, Jennifer;
   James, Alexander
2021cosp...43E.992G    Altcode:
  The Sun produces major eruptions, known as coronal mass ejections,
  from a range of heights in its atmosphere and across a range of
  kinematic and spatial scales. From compact, fast active region
  eruptions to high-altitude, slow stealth CMEs. These eruptions are
  the most energetic phenomena in the Solar System and CMEs that reach
  the Earth can create severe space events. Many studies have now
  shown that magnetic flux ropes are a fundamental component of the
  pre-eruption corona in some cases. In addition, a key role appears
  to be played by magnetic reconnection that evolves the pre-eruption
  corona from a sheared arcade to a flux rope configuration, which can
  then be destabilised by an ideal MHD process or by further magnetic
  reconnection. This talk will look CMEs originating in active regions
  covering the spectrum of events from energetic CMEs to low-energy
  stealth CMEs, and will ask whether there are common processes taking
  place across this wide range and whether flux ropes are involved in
  all cases. A long-term perspective will be given using observational
  and modelling results. The emergence of flux that forms the active
  region will be discussed along with the evolution of this flux via
  photospheric flows. Finally, thought will be given on the role of the
  ambient coronal field on the destabilisation of the CME structure.

---------------------------------------------------------
Title: Alfvénic Perturbations in a Sunspot Chromosphere Linked to
    Fractionated Plasma in the Corona
Authors: Baker, Deborah; Stangalini, Marco; Valori, Gherardo; Brooks,
   David H.; To, Andy S. H.; van Driel-Gesztelyi, Lidia; Démoulin,
   Pascal; Stansby, David; Jess, David B.; Jafarzadeh, Shahin
2021ApJ...907...16B    Altcode: 2020arXiv201204308B
  In this study, 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. We
  find that, in the coronal magnetic field above the sunspot umbra,
  the plasma has photospheric composition. Coronal loops rooted in the
  penumbra contain fractionated plasma, with the highest levels observed
  in the loops that connect within the active region. Tracing field
  lines from regions of fractionated plasma in the corona to locations
  of Alfvénic fluctuations detected in the chromosphere shows that they
  are magnetically linked. These results indicate a connection between
  sunspot chromospheric activity and observable changes in coronal
  plasma composition.

---------------------------------------------------------
Title: Analysis of time-domain correlations between EUV and in-situ
    observations of coronal jets
Authors: de Pablos, D.; Owen, C. J.; Long, D.; Harra, L. K.; Valori,
   G.; Nicolaou, G.
2020AGUFMSH0290018D    Altcode:
  The role of small-scale coronal eruptive phenomena in the origin and
  heating of the solar wind remains an open question. In this work we
  attempt to determine the role played by coronal jets in forming the
  solar wind. This is a challenging problem due to inherent differences
  between remote-sensing observations of the source and in-situ
  observations of the outflowing plasma, as well as its travel time and
  evolution throughout the heliosphere. To overcome these challenges,
  we propose the use of Empirical Mode Decomposition to enable direct
  comparison of temporal signatures within remote sensing observations of
  eruptive phenomena in the corona and in-situ measurements of the solar
  wind. The technique is first validated using artificial data before
  being applied to measurements from the Solar Dynamics Observatory and
  Wind spacecraft. We discuss the potential reasons for discrepancies
  between results from the artificial data and observations at 1 AU,
  and their implications on the solar wind nature.

---------------------------------------------------------
Title: A new trigger mechanism for coronal mass ejections. The role
    of confined flares and photospheric motions in the formation of hot
    flux ropes
Authors: James, A. W.; Green, L. M.; van Driel-Gesztelyi, L.;
   Valori, G.
2020A&A...644A.137J    Altcode: 2020arXiv201011204J
  Context. Many previous studies have shown that the magnetic precursor of
  a coronal mass ejection (CME) takes the form of a magnetic flux rope,
  and a subset of them have become known as "hot flux ropes" due to
  their emission signatures in ∼10 MK plasma. <BR /> Aims: We seek to
  identify the processes by which these hot flux ropes form, with a view
  of developing our understanding of CMEs and thereby improving space
  weather forecasts. <BR /> Methods: Extreme-ultraviolet observations
  were used to identify five pre-eruptive hot flux ropes in the solar
  corona and study how they evolved. Confined flares were observed in the
  hours and days before each flux rope erupted, and these were used as
  indicators of episodic bursts of magnetic reconnection by which each
  flux rope formed. The evolution of the photospheric magnetic field
  was observed during each formation period to identify the process(es)
  that enabled magnetic reconnection to occur in the β &lt; 1 corona and
  form the flux ropes. <BR /> Results: The confined flares were found
  to be homologous events and suggest flux rope formation times that
  range from 18 hours to 5 days. Throughout these periods, fragments of
  photospheric magnetic flux were observed to orbit around each other
  in sunspots where the flux ropes had a footpoint. Active regions
  with right-handed (left-handed) twisted magnetic flux exhibited
  clockwise (anticlockwise) orbiting motions, and right-handed
  (left-handed) flux ropes formed. <BR /> Conclusions: We infer that
  the orbital motions of photospheric magnetic flux fragments about
  each other bring magnetic flux tubes together in the corona, enabling
  component reconnection that forms a magnetic flux rope above a flaring
  arcade. This represents a novel trigger mechanism for solar eruptions
  and should be considered when predicting solar magnetic activity. <P
  />Movies associated to Figs. 4, 8, 12, and 14 are available at <A
  href="https://www.aanda.org/10.1051/0004-6361/202038781/olm">https://www.aanda.org</A>

---------------------------------------------------------
Title: Metis - Solar Orbiter Topical Team on "Modelling of CME
    propagation/evolution in corona and solar wind in connection with
    Space Weather"
Authors: Bemporad, A.; Banerjee, D.; Berlicki, A.; Biondo, R.; Boe,
   B.; Calchetti, D.; Capuano, G.; De Leo, Y.; Del Moro, D.; Feng, L.;
   Foldes, R.; Frassati, F.; Frazin, R. A.; Giovannelli, L.; Giunta,
   A. S.; Heinzel, P.; Ippolito, A.; Janvier, M.; Jerse, G.; Kilpua,
   K. E. J.; Laurenza, M.; Lloveras, D.; Magdalenic, J.; Mancuso, S.;
   Messerotti, M.; Mierla, M.; Nandy, D.; Napoletano, G.; Nuevo, F.;
   Pagano, P.; Pinto, R.; Plainaki, C.; Reale, F.; Romoli, M.; Rodriguez,
   L.; Slemer, A.; Spadaro, D.; Susino, R.; Stangalini, M.; Vainio,
   R. O.; Valori, G.; Vásquez, A. M.; West, M. J.
2020AGUFMSH0360027B    Altcode:
  Despite the current availability of multi-spacecraft observations of
  Coronal Mass Ejections (CMEs) and their interplanetary counterpart
  (ICMEs), at present we still don't understand which physical phenomena
  are driving their expansion and propagation phases. This also limits
  our understanding on how CMEs (observed with remote sensing data)
  become ICMEs (observed in situ), how they interact with the background
  solar wind, and how their final geo-effectiveness can be modified
  during their interplanetary evolution. Such problems match some of
  the scientific objectives of the Solar Orbiter Science Activity Plan
  and of the Metis coronagraph. Thanks to its multi-channel capability,
  Metis (acquiring images in the visible light and at the same time in
  the UV HI Lyman-alpha emission) will really provide an unprecedented
  view of CMEs and in particular of their thermodynamic evolution. At
  closest approaches to the Sun (in the nominal mission), Metis will
  acquire high spatial resolution and/or temporal cadence multi-channel
  images of CMEs. Farther from the Sun, Metis will shed light on the
  early Interplanetary propagation of CMEs. Later on (in the extended
  mission) Metis will observe for the first time the CME/ICME propagation
  out-of-ecliptic. These novelties will be combined with the unique
  vantage point that will be offered by the Solar Orbiter spacecraft,
  and supported with valuable data acquired by other on-board remote
  sensing (e.g. SPICE, EUI, SoloHI) and in situ (e.g. EPD, MAG,
  SWA, RPW) instruments. In this contribution we present the ongoing
  activities of the Metis Topical Team on "CME/ICME propagation", (<A
  href="http://metis.oato.inaf.it/topical_teams.html">http://metis.oato.inaf.it/topical_teams.html</A>),
  an international working group recently established and gathering
  scientists from different countries, experts of both in-situ and remote
  sensing observations, as well as numerical simulations, and we summarize
  the main science objectives discussed during the last months.

---------------------------------------------------------
Title: Additivity of relative magnetic helicity in finite volumes
Authors: Valori, Gherardo; Démoulin, Pascal; Pariat, Etienne; Yeates,
   Anthony; Moraitis, Kostas; Linan, Luis
2020A&A...643A..26V    Altcode: 2020arXiv200800968V
  Context. Relative magnetic helicity is conserved by magneto-hydrodynamic
  evolution even in the presence of moderate resistivity. For that reason,
  it is often invoked as the most relevant constraint on the dynamical
  evolution of plasmas in complex systems, such as solar and stellar
  dynamos, photospheric flux emergence, solar eruptions, and relaxation
  processes in laboratory plasmas. However, such studies often indirectly
  imply that relative magnetic helicity in a given spatial domain can be
  algebraically split into the helicity contributions of the composing
  subvolumes, in other words that it is an additive quantity. A limited
  number of very specific applications have shown that this is not the
  case. <BR /> Aims: Progress in understanding the nonadditivity of
  relative magnetic helicity requires removal of restrictive assumptions
  in favor of a general formalism that can be used in both theoretical
  investigations and numerical applications. <BR /> Methods: We derive the
  analytical gauge-invariant expression for the partition of relative
  magnetic helicity between contiguous finite volumes, without any
  assumptions on either the shape of the volumes and interface, or the
  employed gauge. <BR /> Results: We prove the nonadditivity of relative
  magnetic helicity in finite volumes in the most general, gauge-invariant
  formalism, and verify this numerically. We adopt more restrictive
  assumptions to derive known specific approximations, which yields a
  unified view of the additivity issue. As an example, the case of a
  flux rope embedded in a potential field shows that the nonadditivity
  term in the partition equation is, in general, non-negligible. <BR
  /> Conclusions: The nonadditivity of relative magnetic helicity can
  potentially be a serious impediment to the application of relative
  helicity conservation as a constraint on the complex dynamics of
  magnetized plasmas. The relative helicity partition formula can be
  applied to numerical simulations to precisely quantify the effect of
  nonadditivity on global helicity budgets of complex physical processes.

---------------------------------------------------------
Title: Erratum: "On the Reliability of Magnetic Energy and Helicity
    Computations Based on Nonlinear Force-free Coronal Magnetic Field
    Models" (2019, ApJL, 880, L6)
Authors: Thalmann, Julia K.; Linan, L.; Pariat, E.; Valori, G.
2020ApJ...902L..48T    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Study of the spatial association between an active region
    jet and a nonthermal type~${\rm III}$ radio burst
Authors: Mulay, Sargam M.; Sharma, Rohit; Valori, Gherardo; Vásquez,
   Alberto M.; Del Zanna, Giulio; Mason, Helen; Oberoi, Divya
2020arXiv200914581M    Altcode:
  We aim to investigate the spatial location of the source of an active
  region (AR) jet and its relation with associated nonthermal type~III
  radio emission. An emission measure (EM) method was used to study
  the thermodynamic nature of the AR jet. The nonthermal type~{\rm III}
  radio burst observed at meterwavelength was studied using the Murchison
  Widefield Array (MWA) radio imaging and spectroscopic data. The local
  configuration of the magnetic field and the connectivity of the source
  region of the jet with open magnetic field structures was studied using
  a nonlinear force-free field (NLFFF) extrapolation and potential field
  source surface (PFSS) extrapolation respectively. The plane-of-sky
  velocity of the AR jet was found to be $\sim$136~km/s. The EM analysis
  confirmed the presence of low temperature 2~MK plasma for the spire,
  whereas hot plasma, between 5-8 MK, was present at the footpoint region
  which also showed the presence of Fe~{\sc xviii} emission. A lower limit
  on the electron number density was found to be 1.4$\times$10$^{8}$
  cm$^{-3}$ for the spire and 2.2$\times$10$^{8}$~cm$^{-3}$ for
  the footpoint. A temporal and spatial correlation between the AR
  jet and nonthermal type III burst confirmed the presence of open
  magnetic fields. An NLFFF extrapolation showed that the photospheric
  footpoints of the null point were anchored at the location of the
  source brightening of the jet. The spatial location of the radio
  sources suggests an association with the extrapolated closed and
  open magnetic fields although strong propagation effects are also
  present. The multi-scale analysis of the field at local, AR, and solar
  scales confirms the interlink between different flux bundles involved
  in the generation of the type III radio signal with flux transferred
  from a small coronal hole to the periphery of the sunspot via null
  point reconnection with an emerging structure.

---------------------------------------------------------
Title: The Magnetic Environment of a Stealth CME
Authors: O'Kane, J.; Mandrini, C.; Demoulin, P.; Green, L.; Valori,
   G.; Long, D.
2020SPD....5121005O    Altcode:
  Interest in Stealth Coronal Mass Ejections (CMEs) is increasing due to
  their relatively high occurrence rate and space weather impact. However,
  typical CME signatures such as EUV dimmings and post-eruptive arcades
  are hard to identify for stealth CMEs and require extensive image
  processing techniques. These weak observational signatures mean little
  is currently understood about the physics of these events. We present
  an extensive study of the magnetic field configuration in which the
  stealth CME of 3 March 2011 occurred. The magnetic field prior to the
  eruption is evaluated using a Linear Force Free Field (LFFF) model
  and a Potential Field Source Surface (PFSS) model, and complemented
  by in-depth observational analysis. The models are verified using
  observations of plasma emission structures in the stealth CME source
  region and trans-equatorial loops. We find evidence of a high-altitude
  null point in both the LFFF model and the PFSS model, with surrounding
  field lines connecting two active regions on the solar disk. One of
  these active regions in the Southern Hemisphere is shown to be the
  source region of the stealth CME. Three distinct episodes of flare
  ribbon formation are observed in AIA 304Å. Two occurred prior to
  the eruption and suggest the occurrence of magnetic reconnection that
  builds the eruptive structure. The third occurs at the same time as an
  erupting cavity is observed in STEREO-B 171Å data; this subsequently
  becomes part of the propagating CME observed in COR1. We conclude that
  reconnection at the null point, driven by eruptive activity in the
  complex northern active region, aids the eruption of the stealth CME
  by removing field that acted to stabilise the pre-eruptive structure.

---------------------------------------------------------
Title: Modelado magnético de regiones activas solares: Una
    comparación entre dos modelos libres de fuerzas
Authors: Nuevo, F. A.; Valori, G.; López Fuentes, M.; Mandrini,
   C. H.; Vásquez, A. M.
2020BAAA...61B...7N    Altcode:
  The knowledge of the three-dimensional coronal magnetic field
  ($\mathbf{B}$) at high spatial resolution is key to better understand
  the physical mechanisms that trigger active phenomena in the corona,
  the main drivers of { space weather}. High resolution, direct coronal
  measurements of $\mathbf{B}$ are not available, so we must rely on
  suitable coronal field models based on the available photospheric field
  measurements (magnetograms). For active region (AR) magnetic fields,
  where { magnetic pressure is much larger than plasma pressure}, the
  force-free regime ($\nabla\times\mathbf{B} = \alpha \mathbf{B}$) is
  a valid approximation. Force-free field models for which the $\alpha$
  parameter is a constant are called Linear (LFFF) and models for which
  $\alpha$ is a function of { the} position are called non-linear
  (NLFFF).In this work we test and compare specific numerical
  implementations of both LFFF and NLFFF models applied to two ARs.

---------------------------------------------------------
Title: Can Subphotospheric Magnetic Reconnection Change the Elemental
    Composition in the Solar Corona?
Authors: Baker, Deborah; van Driel-Gesztelyi, Lidia; Brooks, David H.;
   Démoulin, Pascal; Valori, Gherardo; Long, David M.; Laming, J. Martin;
   To, Andy S. H.; James, Alexander W.
2020ApJ...894...35B    Altcode: 2020arXiv200303325B
  Within the coronae of stars, abundances of those elements with low
  first ionization potential (FIP) often differ from their photospheric
  values. The coronae of the Sun and solar-type stars mostly show
  enhancements of low-FIP elements (the FIP effect) while more active
  stars such as M dwarfs have coronae generally characterized by the
  inverse-FIP effect (I-FIP). Here we observe patches of I-FIP effect
  solar plasma in AR 12673, a highly complex βγδ active region. We
  argue that the umbrae of coalescing sunspots, and more specifically
  strong light bridges within the umbrae, are preferential locations for
  observing I-FIP effect plasma. Furthermore, the magnetic complexity
  of the active region and major episodes of fast flux emergence also
  lead to repetitive and intense flares. The induced evaporation of
  the chromospheric plasma in flare ribbons crossing umbrae enables
  the observation of four localized patches of I-FIP effect plasma in
  the corona of AR 12673. These observations can be interpreted in the
  context of the ponderomotive force fractionation model which predicts
  that plasma with I-FIP effect composition is created by the refraction
  of waves coming from below the chromosphere. We propose that the waves
  generating the I-FIP effect plasma in solar active regions are generated
  by subphotospheric reconnection of coalescing flux systems. Although
  we only glimpse signatures of I-FIP effect fractionation produced by
  this interaction in patches on the Sun, on highly active M stars it
  may be the dominant process.

---------------------------------------------------------
Title: Energy and helicity fluxes in line-tied eruptive simulations
Authors: Linan, L.; Pariat, É.; Aulanier, G.; Moraitis, K.; Valori, G.
2020A&A...636A..41L    Altcode: 2020arXiv200301698L
  Context. Conservation properties of magnetic helicity and energy in
  the quasi-ideal and low-β solar corona make these two quantities
  relevant for the study of solar active regions and eruptions. <BR />
  Aims: Based on a decomposition of the magnetic field into potential
  and nonpotential components, magnetic energy and relative helicity
  can both also be decomposed into two quantities: potential and free
  energies, and volume-threading and current-carrying helicities. In
  this study, we perform a coupled analysis of their behaviors in a set
  of parametric 3D magnetohydrodynamic (MHD) simulations of solar-like
  eruptions. <BR /> Methods: We present the general formulations for
  the time-varying components of energy and helicity in resistive
  MHD. We calculated them numerically with a specific gauge, and
  compared their behaviors in the numerical simulations, which differ
  from one another by their imposed boundary-driving motions. Thus,
  we investigated the impact of different active regions surface flows
  on the development of the energy and helicity-related quantities. <BR
  /> Results: Despite general similarities in their overall behaviors,
  helicities and energies display different evolutions that cannot be
  explained in a unique framework. While the energy fluxes are similar
  in all simulations, the physical mechanisms that govern the evolution
  of the helicities are markedly distinct from one simulation to another:
  the evolution of volume-threading helicity can be governed by boundary
  fluxes or helicity transfer, depending on the simulation. <BR />
  Conclusions: The eruption takes place for the same value of the
  ratio of the current-carrying helicity to the total helicity in all
  simulations. However, our study highlights that this threshold can be
  reached in different ways, with different helicity-related processes
  dominating for different photospheric flows. This means that the
  details of the pre-eruptive dynamics do not influence the eruption-onset
  helicity-related threshold. Nevertheless, the helicity-flux dynamics
  may be more or less efficient in changing the time required to reach
  the onset of the eruption.

---------------------------------------------------------
Title: Study of the spatial association between an active region
    jet and a nonthermal type III radio burst
Authors: Mulay, Sargam M.; Sharma, Rohit; Valori, Gherardo; Vásquez,
   Alberto M.; Del Zanna, Giulio; Mason, Helen; Oberoi, Divya
2019A&A...632A.108M    Altcode:
  <BR /> Aims: We aim to investigate the spatial location of the source
  of an active region (AR) jet and its relation with associated nonthermal
  type III radio emission. <BR /> Methods: An emission measure (EM) method
  was used to study the thermodynamic nature of the AR jet. The nonthermal
  type III radio burst observed at meterwavelength was studied using
  the Murchison Widefield Array (MWA) radio imaging and spectroscopic
  data. The local configuration of the magnetic field and the connectivity
  of the source region of the jet with open magnetic field structures was
  studied using a nonlinear force-free field (NLFFF) extrapolation and
  potential field source surface (PFSS) extrapolation respectively. <BR
  /> Results: The plane-of-sky velocity of the AR jet was found to be
  ∼136 km s<SUP>-1</SUP>. The EM analysis confirmed the presence of
  low temperature 2 MK plasma for the spire, whereas hot plasma, between
  5 and 8 MK, was present at the footpoint region which also showed the
  presence of Fe XVIII emission. A lower limit on the electron number
  density was found to be 1.4 × 10<SUP>8</SUP> cm<SUP>-3</SUP> for the
  spire and 2.2 × 10<SUP>8</SUP> cm<SUP>-3</SUP> for the footpoint. A
  temporal and spatial correlation between the AR jet and nonthermal
  type III burst confirmed the presence of open magnetic fields. An NLFFF
  extrapolation showed that the photospheric footpoints of the null point
  were anchored at the location of the source brightening of the jet. The
  spatial location of the radio sources suggests an association with the
  extrapolated closed and open magnetic fields although strong propagation
  effects are also present. <BR /> Conclusions: The multi-scale analysis
  of the field at local, AR, and solar scales confirms the interlink
  between different flux bundles involved in the generation of the type
  III radio signal with flux transferred from a small coronal hole to the
  periphery of the sunspot via null point reconnection with an emerging
  structure. <P />The movie associated to Fig. 4 is available at <A
  href="https://www.aanda.org/10.1051/0004-6361/201936369/olm">https://www.aanda.org</A>

---------------------------------------------------------
Title: Magnetic Helicity Budget of Solar Active Regions Prolific of
    Eruptive and Confined Flares
Authors: Thalmann, Julia K.; Moraitis, K.; Linan, L.; Pariat, E.;
   Valori, G.; Dalmasse, K.
2019ApJ...887...64T    Altcode: 2019arXiv191006563T
  We compare the coronal magnetic energy and helicity of two solar active
  regions (ARs), prolific in major eruptive (AR 11158) and confined
  (AR 12192) flaring, and analyze the potential of deduced proxies
  to forecast upcoming flares. Based on nonlinear force-free (NLFF)
  coronal magnetic field models with a high degree of solenoidality,
  and applying three different computational methods to investigate
  the coronal magnetic helicity, we are able to draw conclusions
  with a high level of confidence. Based on real observations of two
  solar ARs we checked trends regarding the potential eruptivity of
  the active-region corona, as suggested earlier in works that were
  based on numerical simulations, or solar observations. Our results
  support that the ratio of current-carrying to total helicity, |
  {H}<SUB>{{J</SUB>}}| /| {H}<SUB>{ \mathcal V </SUB>}| , shows a strong
  ability to indicate the eruptive potential of a solar AR. However, |
  {H}<SUB>{{J</SUB>}}| /| {H}<SUB>{ \mathcal V </SUB>}| does not seem to
  be indicative for the magnitude or type of an upcoming flare (confined
  or eruptive). Interpreted in the context of earlier observational
  studies, our findings furthermore support that the total relative
  helicity normalized to the magnetic flux at the NLFF model’s lower
  boundary, {H}<SUB>{ \mathcal V </SUB>}/{φ }<SUP>2</SUP>, represents
  no indicator for the eruptivity.

---------------------------------------------------------
Title: Quantifying the Relationship between Moreton-Ramsey Waves
    and “EIT Waves” Using Observations of Four Homologous Wave Events
Authors: Long, David M.; Jenkins, Jack; Valori, Gherardo
2019ApJ...882...90L    Altcode: 2019arXiv190707963L
  Freely propagating global waves in the solar atmosphere are commonly
  observed using extreme ultraviolet passbands (EUV or “EIT waves”),
  and less regularly in H-alpha (Moreton-Ramsey waves). Despite
  decades of research, joint observations of EUV and Moreton-Ramsey
  waves remain rare, complicating efforts to quantify the connection
  between these phenomena. We present observations of four homologous
  global waves originating from the same active region between 2014
  March 28 and 30 and observed using both EUV and H-alpha data. Each
  global EUV wave was observed by the Solar Dynamics Observatory,
  with the associated Moreton-Ramsey waves identified using the Global
  Oscillations Network Group network. All of the global waves exhibit
  high initial velocity (e.g., 842-1388 km s<SUP>-1</SUP> in the 193 Å
  passband) and strong deceleration (e.g., -1437 to -782 m s<SUP>-2</SUP>
  in the 193 Å passband) in each of the EUV passbands studied, with the
  EUV wave kinematics exceeding those of the Moreton-Ramsey wave. The
  density compression ratio of each global wave was estimated using both
  differential emission measure and intensity variation techniques, with
  both indicating that the observed waves were weakly shocked with a fast
  magnetosonic Mach number slightly greater than one. This suggests that,
  according to current models, the global coronal waves were not strong
  enough to produce Moreton-Ramsey waves, indicating an alternative
  explanation for these observations. Instead, we conclude that the
  evolution of the global waves was restricted by the surrounding
  coronal magnetic field, in each case producing a downward-angled
  wavefront propagating toward the north solar pole, which perturbed
  the chromosphere and was observed as a Moreton-Ramsey wave.

---------------------------------------------------------
Title: On the Reliability of Magnetic Energy and Helicity Computations
    Based on Nonlinear Force-free Coronal Magnetic Field Models
Authors: Thalmann, Julia K.; Linan, L.; Pariat, E.; Valori, G.
2019ApJ...880L...6T    Altcode: 2019arXiv190701179T
  We demonstrate the sensitivity of magnetic energy and helicity
  computations regarding the quality of the underlying coronal magnetic
  field model. We apply the method of Wiegelmann &amp; Inhester to a
  series of Solar Dynamics Observatory/Helioseismic and Magnetic Imager
  vector magnetograms, and discuss nonlinear force-free (NLFF) solutions
  based on two different sets of the free model parameters. The two
  time series differ from each other concerning their force-free and
  solenoidal quality. Both force- and divergence-freeness are required
  for a consistent NLFF solution. Full satisfaction of the solenoidal
  property is inherent in the definition of relative magnetic helicity
  in order to ensure gauge independence. We apply two different magnetic
  helicity computation methods to both NLFF time series and find that
  the output is highly dependent on the level to which the NLFF magnetic
  fields satisfy the divergence-free condition, with the computed magnetic
  energy being less sensitive than the relative helicity. Proxies for
  the nonpotentiality and eruptivity derived from both quantities are
  also shown to depend strongly on the solenoidal property of the NLFF
  fields. As a reference for future applications, we provide quantitative
  thresholds for the force- and divergence-freeness, for the assurance
  of reliable computation of magnetic energy and helicity, and of their
  related eruptivity proxies.

---------------------------------------------------------
Title: Relative magnetic field line helicity
Authors: Moraitis, K.; Pariat, E.; Valori, G.; Dalmasse, K.
2019A&A...624A..51M    Altcode: 2019arXiv190210410M
  Context. Magnetic helicity is an important quantity in studies
  of magnetized plasmas as it provides a measure of the geometrical
  complexity of the magnetic field in a given volume. A more detailed
  description of the spatial distribution of magnetic helicity is given
  by the field line helicity, which expresses the amount of helicity
  associated to individual field lines rather than in the full analysed
  volume. <BR /> Aims: Magnetic helicity is not a gauge-invariant quantity
  in general, unless it is computed with respect to a reference field,
  yielding the so-called relative magnetic helicity. The field line
  helicity corresponding to the relative magnetic helicity has only been
  examined under specific conditions so far. This work aims to define
  the field line helicity corresponding to relative magnetic helicity
  in the most general way. In addition to its general form, we provide
  the expression for the relative magnetic field line helicity in a few
  commonly used gauges, and reproduce known results as a limit of our
  general formulation. <BR /> Methods: By starting from the definition
  of relative magnetic helicity, we derived the corresponding field line
  helicity, and we noted the assumptions on which it is based. <BR />
  Results: We checked that the developed quantity reproduces relative
  magnetic helicity by using three different numerical simulations. For
  these cases we also show the morphology of field line helicity in
  the volume, and on the photospheric plane. As an application to solar
  situations, we compared the morphology of field line helicity on the
  photosphere with that of the connectivity-based helicity flux density
  in two reconstructions of an active region's magnetic field. We
  discuss how the derived relative magnetic field line helicity has
  a wide range of applications, notably in solar physics and magnetic
  reconnection studies.

---------------------------------------------------------
Title: Transient Inverse-FIP Plasma Composition Evolution within a
    Solar Flare
Authors: Baker, Deborah; van Driel-Gesztelyi, Lidia; Brooks, David
   H.; Valori, Gherardo; James, Alexander W.; Laming, J. Martin; Long,
   David M.; Démoulin, Pascal; Green, Lucie M.; Matthews, Sarah A.;
   Oláh, Katalin; Kővári, Zsolt
2019ApJ...875...35B    Altcode: 2019arXiv190206948B
  Understanding elemental abundance variations in the solar corona
  provides an insight into how matter and energy flow from the
  chromosphere into the heliosphere. Observed variations depend on the
  first ionization potential (FIP) of the main elements of the Sun’s
  atmosphere. High-FIP elements (&gt;10 eV) maintain photospheric
  abundances in the corona, whereas low-FIP elements have enhanced
  abundances. Conversely, inverse FIP (IFIP) refers to the enhancement of
  high-FIP or depletion of low-FIP elements. We use spatially resolved
  spectroscopic observations, specifically the Ar XIV/Ca XIV intensity
  ratio, from Hinode’s Extreme-ultraviolet Imaging Spectrometer to
  investigate the distribution and evolution of plasma composition
  within two confined flares in a newly emerging, highly sheared
  active region. During the decay phase of the first flare, patches
  above the flare ribbons evolve from the FIP to the IFIP effect, while
  the flaring loop tops show a stronger FIP effect. The patch and loop
  compositions then evolve toward the preflare basal state. We propose
  an explanation of how flaring in strands of highly sheared emerging
  magnetic fields can lead to flare-modulated IFIP plasma composition
  over coalescing umbrae which are crossed by flare ribbons. Subsurface
  reconnection between the coalescing umbrae leads to the depletion of
  low-FIP elements as a result of an increased wave flux from below. This
  material is evaporated when the flare ribbons cross the umbrae. Our
  results are consistent with the ponderomotive fractionation model for
  the creation of IFIP-biased plasma.

---------------------------------------------------------
Title: Modeling the Effect of Mass-draining on Prominence Eruptions
Authors: Jenkins, Jack M.; Hopwood, Matthew; Démoulin, Pascal; Valori,
   Gherardo; Aulanier, Guillaume; Long, David M.; van Driel-Gesztelyi,
   Lidia
2019ApJ...873...49J    Altcode: 2019arXiv190110970J
  Quiescent solar prominences are observed within the solar atmosphere
  for up to several solar rotations. Their eruption is commonly preceded
  by a slow increase in height that can last from hours to days. This
  increase in the prominence height is believed to be due to their host
  magnetic flux rope transitioning through a series of neighboring
  quasi-equilibria before the main loss of equilibrium that drives
  the eruption. Recent work suggests that the removal of prominence
  mass from a stable, quiescent flux rope is one possible cause for
  this change in height. However, these conclusions are drawn from
  observations and are subject to interpretation. Here, we present a
  simple model to quantify the effect of “mass-draining” during the
  pre-eruptive height evolution of a solar flux rope. The flux rope is
  modeled as a line current suspended within a background potential
  magnetic field. We first show that the inclusion of mass, up to
  10<SUP>12</SUP> kg, can modify the height at which the line current
  experiences loss of equilibrium by up to 14%. Next, we show that
  the rapid removal of mass prior to the loss of equilibrium can allow
  the height of the flux rope to increase sharply and without an upper
  bound as it approaches its loss-of-equilibrium point. This indicates
  that the critical height for the loss of equilibrium can occur at a
  range of heights depending explicitly on the amount and evolution of
  mass within the flux rope. Finally, we demonstrate that for the same
  amount of drained mass, the effect on the height of the flux rope is
  up to two orders of magnitude larger for quiescent prominences than
  for active region prominences.

---------------------------------------------------------
Title: An Observationally Constrained Model of a Flux Rope that
    Formed in the Solar Corona
Authors: James, Alexander W.; Valori, Gherardo; Green, Lucie M.; Liu,
   Yang; Cheung, Mark C. M.; Guo, Yang; van Driel-Gesztelyi, Lidia
2018csc..confE...9J    Altcode:
  Coronal mass ejections (CMEs) are large-scale eruptions of plasma
  from the coronae of stars, and it is important to study the plasma
  processes involved in their initiation. This first requires us to
  understand the pre-eruptive configuration of CMEs. To this end, we used
  extreme-ultraviolet (EUV) observations from SDO/AIA to conclude that a
  magnetic flux rope formed high-up in the solar corona above NOAA Active
  Region 11504 before it erupted on 2012 June 14. Then, we used data from
  SDO/HMI and our knowledge of the EUV observations to model the coronal
  magnetic field of the active region one hour prior to eruption using a
  nonlinear force-free field extrapolation. The extrapolation revealed
  a flux rope that matches the EUV observations remarkably well, with
  its axis 120 Mm above the photosphere. The erupting structure was not
  observed to kink, but the decay index near the apex of the axis of
  the extrapolated flux rope is comparable to typical critical values
  required for the onset of the torus instability. Therefore, we suggest
  that the torus instability drove the eruption of the flux rope.

---------------------------------------------------------
Title: Multi-wavelength observations of 4 homologous global coronal
    waves
Authors: Long, David; Lawless, Julia; Valori, Gherardo; Jenkins, Jack
2018csc..confE..15L    Altcode:
  Global coronal waves (commonly called "EIT waves") were first observed
  by SOHO/EIT in 1997 and are now considered to be large-scale shock
  fronts initially driven by the rapid expansion of an erupting coronal
  mass ejection in the low corona. I will present observations of four
  homologous global waves which erupted from the same active region over
  the course of three days in March 2014. Each global EUV wave was well
  observed by SDO/AIA and was associated with a H-alpha Moreton-Ramsey
  wave observed at high cadence by the GONG network. These observations
  provide the opportunity to directly relate global waves in EUV and
  H-alpha observations with high cadence and answer a fundamental
  question about the relationship between these phenomena which has
  persisted since they were first observed.

---------------------------------------------------------
Title: Time Variations of the Nonpotential and Volume-threading
    Magnetic Helicities
Authors: Linan, L.; Pariat, É.; Moraitis, K.; Valori, G.; Leake, J.
2018ApJ...865...52L    Altcode: 2018arXiv180903765L
  Relative magnetic helicity is a gauge-invariant quantity suitable
  for the study of the magnetic helicity content of heliospheric
  plasmas. Relative magnetic helicity can be decomposed uniquely
  into two gauge-invariant quantities, the magnetic helicity
  of the nonpotential component of the field and a complementary
  volume-threading helicity. Recent analysis of numerical experiments
  simulating the generation of solar eruptions have shown that the
  ratio of the nonpotential helicity to the total relative helicity is
  a clear marker of the eruptivity of the magnetic system, and that the
  high value of that quantity could be a sufficient condition for the
  onset of the instability generating the eruptions. The present study
  introduces the first analytical examination of the time variations
  of these nonpotential and volume-threading helicities. The validity
  of the analytical formulae derived are confirmed with analysis of 3D
  magnetohydrodynamics (MHD) simulations of solar coronal dynamics. Both
  the analytical investigation and the numerical application show that,
  unlike magnetic helicity, the nonpotential and the volume-threading
  helicities are not conserved quantities, even in the ideal MHD regime. A
  term corresponding to the transformation between the nonpotential and
  volume-threading helicities frequently dominates their dynamics. This
  finding has an important consequence for their estimation in the
  solar corona: unlike with relative helicity, their volume coronal
  evolution cannot be ascertained by the flux of these quantities
  through the volume’s boundaries. Only techniques extrapolating the
  3D coronal field will enable both the proper study of the nonpotential
  and volume-threading helicities and the observational analysis of
  helicity-based solar-eruptivity proxies.

---------------------------------------------------------
Title: Threshold of Non-potential Magnetic Helicity Ratios at the
    Onset of Solar Eruptions
Authors: Zuccarello, F. P.; Pariat, E.; Valori, G.; Linan, L.
2018ApJ...863...41Z    Altcode: 2018arXiv180700532Z
  The relative magnetic helicity is a quantity that is often used to
  describe the level of entanglement of non-isolated magnetic fields,
  such as the magnetic field of solar active regions. The aim of this
  paper is to investigate how different kinds of photospheric boundary
  flows accumulate relative magnetic helicity in the corona and if and
  how well magnetic-helicity-related quantities identify the onset
  of an eruption. We use a series of three-dimensional, parametric
  magnetohydrodynamic simulations of the formation and eruption of
  magnetic flux ropes. All the simulations are performed on the same
  grid, using the same parameters, but they are characterized by different
  driving photospheric flows, i.e., shearing, convergence, stretching, and
  peripheral- and central- dispersion flows. For each of the simulations,
  the instant of the onset of the eruption is carefully identified
  by using a series of relaxation runs. We find that magnetic energy
  and total relative helicity are mostly injected when shearing flows
  are applied at the boundary, while the magnetic energy and helicity
  associated with the coronal electric currents increase regardless of
  the kind of photospheric flows. We also find that, at the onset of
  the eruptions, the ratio between the non-potential magnetic helicity
  and the total relative magnetic helicity has the same value for all
  the simulations, suggesting the existence of a threshold in this
  quantity. Such a threshold is not observed for other quantities as,
  for example, those related to the magnetic energy.

---------------------------------------------------------
Title: Computation of Relative Magnetic Helicity in Spherical
    Coordinates
Authors: Moraitis, Kostas; Pariat, Étienne; Savcheva, Antonia;
   Valori, Gherardo
2018SoPh..293...92M    Altcode: 2018arXiv180603011M
  Magnetic helicity is a quantity of great importance in solar studies
  because it is conserved in ideal magnetohydrodynamics. While many
  methods for computing magnetic helicity in Cartesian finite volumes
  exist, in spherical coordinates, the natural coordinate system
  for solar applications, helicity is only treated approximately. We
  present here a method for properly computing the relative magnetic
  helicity in spherical geometry. The volumes considered are finite,
  of shell or wedge shape, and the three-dimensional magnetic field is
  considered to be fully known throughout the studied domain. Testing of
  the method with well-known, semi-analytic, force-free magnetic-field
  models reveals that it has excellent accuracy. Further application to
  a set of nonlinear force-free reconstructions of the magnetic field of
  solar active regions and comparison with an approximate method used
  in the past indicates that the proposed method can be significantly
  more accurate, thus making our method a promising tool in helicity
  studies that employ spherical geometry. Additionally, we determine
  and discuss the applicability range of the approximate method.

---------------------------------------------------------
Title: An Observationally Constrained Model of a Flux Rope that
    Formed in the Solar Corona
Authors: James, Alexander W.; Valori, Gherardo; Green, Lucie M.; Liu,
   Yang; Cheung, Mark C. M.; Guo, Yang; van Driel-Gesztelyi, Lidia
2018ApJ...855L..16J    Altcode: 2018arXiv180207965J
  Coronal mass ejections (CMEs) are large-scale eruptions of plasma
  from the coronae of stars. Understanding the plasma processes involved
  in CME initiation has applications for space weather forecasting and
  laboratory plasma experiments. James et al. used extreme-ultraviolet
  (EUV) observations to conclude that a magnetic flux rope formed in
  the solar corona above NOAA Active Region 11504 before it erupted on
  2012 June 14 (SOL2012-06-14). In this work, we use data from the Solar
  Dynamics Observatory (SDO) to model the coronal magnetic field of the
  active region one hour prior to eruption using a nonlinear force-free
  field extrapolation, and find a flux rope reaching a maximum height
  of 150 Mm above the photosphere. Estimations of the average twist of
  the strongly asymmetric extrapolated flux rope are between 1.35 and
  1.88 turns, depending on the choice of axis, although the erupting
  structure was not observed to kink. The decay index near the apex
  of the axis of the extrapolated flux rope is comparable to typical
  critical values required for the onset of the torus instability,
  so we suggest that the torus instability drove the eruption.

---------------------------------------------------------
Title: Studying the Transfer of Magnetic Helicity in Solar Active
    Regions with the Connectivity-based Helicity Flux Density Method
Authors: Dalmasse, K.; Pariat, É.; Valori, G.; Jing, J.; Démoulin, P.
2018ApJ...852..141D    Altcode: 2017arXiv171204691D
  In the solar corona, magnetic helicity slowly and continuously
  accumulates in response to plasma flows tangential to the photosphere
  and magnetic flux emergence through it. Analyzing this transfer of
  magnetic helicity is key for identifying its role in the dynamics of
  active regions (ARs). The connectivity-based helicity flux density
  method was recently developed for studying the 2D and 3D transfer
  of magnetic helicity in ARs. The method takes into account the 3D
  nature of magnetic helicity by explicitly using knowledge of the
  magnetic field connectivity, which allows it to faithfully track the
  photospheric flux of magnetic helicity. Because the magnetic field is
  not measured in the solar corona, modeled 3D solutions obtained from
  force-free magnetic field extrapolations must be used to derive the
  magnetic connectivity. Different extrapolation methods can lead to
  markedly different 3D magnetic field connectivities, thus questioning
  the reliability of the connectivity-based approach in observational
  applications. We address these concerns by applying this method to the
  isolated and internally complex AR 11158 with different magnetic field
  extrapolation models. We show that the connectivity-based calculations
  are robust to different extrapolation methods, in particular with
  regard to identifying regions of opposite magnetic helicity flux. We
  conclude that the connectivity-based approach can be reliably used in
  observational analyses and is a promising tool for studying the transfer
  of magnetic helicity in ARs and relating it to their flaring activity.

---------------------------------------------------------
Title: Non-thermal distributions and energy transport in the solar
    flares
Authors: Matthews, Sarah; del Zanna, Guilio; Calcines, Ariadna;
   Mason, Helen; Mathioudakis, Mihalis; Culhane, Len; Harra, Louise;
   van Driel-Gesztelyi, Lidia; Green, Lucie; Long, David; Baker, Deb;
   Valori, Gherardo
2017arXiv171200773M    Altcode:
  Determining the energy transport mechanisms in flares remains a central
  goal in solar flares physics that is still not adequately answered
  by the 'standard flare model'. In particular, the relative roles of
  particles and/or waves as transport mechanisms, the contributions of low
  energy protons and ions to the overall flare budget, and the limits of
  low energy non-thermal electron distribution are questions that still
  cannot be adequately reconciled with current instrumentation. In this
  'White Paper' submitted in response to the call for inputs to the Next
  Generation Solar Physics Mission review process initiated by JAXA,
  NASA and ESA in 2016, we outline the open questions in this area and
  possible instrumentation that could provide the required observations
  to help answer these and other flare-related questions.

---------------------------------------------------------
Title: Measuring the magnetic field of a trans-equatorial loop system
    using coronal seismology (Corrigendum)
Authors: Long, D. M.; Valori, G.; Pérez-Suárez, D.; Morton, R. J.;
   Vásquez, A. M.
2017A&A...607C...3L    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: The 2013 February 17 Sunquake in the Context of the Active
    Region's Magnetic Field Configuration
Authors: Green, L. M.; Valori, G.; Zuccarello, F. P.; Zharkov, S.;
   Matthews, S. A.; Guglielmino, S. L.
2017ApJ...849...40G    Altcode: 2017arXiv170904874G
  Sunquakes are created by the hydrodynamic response of the lower
  atmosphere to a sudden deposition of energy and momentum. In this study,
  we investigate a sunquake that occurred in NOAA active region 11675
  on 2013 February 17. Observations of the corona, chromosphere, and
  photosphere are brought together for the first time with a nonlinear
  force-free model of the active region’s magnetic field in order to
  probe the magnetic environment in which the sunquake was initiated. We
  find that the sunquake was associated with the destabilization of a
  flux rope and an associated M-class GOES flare. Active region 11675
  was in its emergence phase at the time of the sunquake and photospheric
  motions caused by the emergence heavily modified the flux rope and its
  associated quasi-separatrix layers, eventually triggering the flux
  rope’s instability. The flux rope was surrounded by an extended
  envelope of field lines rooted in a small area at the approximate
  position of the sunquake. We argue that the configuration of the
  envelope, by interacting with the expanding flux rope, created a
  “magnetic lens” that may have focussed energy on one particular
  location of the photosphere, creating the necessary conditions for
  the initiation of the sunquake.

---------------------------------------------------------
Title: Flux rope, hyperbolic flux tube, and late extreme ultraviolet
    phases in a non-eruptive circular-ribbon flare
Authors: Masson, Sophie; Pariat, Étienne; Valori, Gherardo; Deng,
   Na; Liu, Chang; Wang, Haimin; Reid, Hamish
2017A&A...604A..76M    Altcode: 2017arXiv170401450M
  Context. The dynamics of ultraviolet (UV) emissions during solar flares
  provides constraints on the physical mechanisms involved in the trigger
  and the evolution of flares. In particular it provides some information
  on the location of the reconnection sites and the associated magnetic
  fluxes. In this respect, confined flares are far less understood
  than eruptive flares generating coronal mass ejections. <BR /> Aims:
  We present a detailed study of a confined circular flare dynamics
  associated with three UV late phases in order to understand more
  precisely which topological elements are present and how they constrain
  the dynamics of the flare. <BR /> Methods: We perform a non-linear
  force-free field extrapolation of the confined flare observed with the
  Helioseismic and Magnetic Imager (HMI) and Atmospheric Imaging Assembly
  (AIA) instruments on board Solar Dynamics Observatory (SDO). From the
  3D magnetic field we compute the squashing factor and we analyse its
  distribution. Conjointly, we analyse the AIA extreme ultraviolet (EUV)
  light curves and images in order to identify the post-flare loops,
  and their temporal and thermal evolution. By combining the two analyses
  we are able to propose a detailed scenario that explains the dynamics
  of the flare. <BR /> Results: Our topological analysis shows that in
  addition to a null-point topology with the fan separatrix, the spine
  lines and its surrounding quasi-separatix layer (QSL) halo (typical
  for a circular flare), a flux rope and its hyperbolic flux tube (HFT)
  are enclosed below the null. By comparing the magnetic field topology
  and the EUV post-flare loops we obtain an almost perfect match between
  the footpoints of the separatrices and the EUV 1600 Å ribbons and
  between the HFT field line footpoints and bright spots observed inside
  the circular ribbons. We show, for the first time in a confined flare,
  that magnetic reconnection occurred initially at the HFT below the flux
  rope. Reconnection at the null point between the flux rope and the
  overlying field is only initiated in a second phase. In addition, we
  showed that the EUV late phase observed after the main flare episode
  is caused by the cooling loops of different length which have all
  reconnected at the null point during the impulsive phase. <BR />
  Conclusions: Our analysis shows in one example that flux ropes are
  present in null-point topology not only for eruptive and jet events,
  but also for confined flares. This allows us to conjecture on the
  analogies between conditions that govern the generation of jets,
  confined flares or eruptive flares. <P />A movie is available at <A
  href="http://www.aanda.org/10.1051/0004-6361/201629654/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: Studying the transfer of magnetic helicity in solar active
    regions
Authors: Dalmasse, Kevin; Valori, Gherardo; Jing, Ju; Pariat, Etienne;
   Demoulin, Pascal
2017SPD....4811206D    Altcode:
  Analyzing the transfer of magnetic helicity in active regions is a
  key component for understanding the nature of its coronal storage
  and release and for identifying its role in the coronal dynamics
  of active regions. We recently developed a method for studying the
  photospheric flux of magnetic helicity in both 2D and 3D. The method
  takes into account the 3D nature of magnetic helicity by explicitly
  using knowledge of the magnetic field connectivity. Since the coronal
  magnetic field in active regions is not measured, we rely on the
  non-unique 3D solution obtained from force-free coronal magnetic
  field extrapolations to derive the magnetic field connectivity. In
  this poster, we apply the method to the complex and highly-flaring
  active region NOAA 11158 using the magnetic field connectivity derived
  from different force-free extrapolation models and implementations. We
  show that the calculations of photospheric flux of magnetic helicity
  are robust to different extrapolation methods and assumptions, in
  particular with regards to identifying regions of opposite magnetic
  helicity flux. Finally, we discuss the implications of our results
  for tracking the transfer of magnetic helicity in active regions and
  relate it to their flaring activity.

---------------------------------------------------------
Title: Studying the transfer of magnetic helicity in solar active
    regions
Authors: Dalmasse, Kévin; Jing, J.; Pariat, E.; Valori, G.;
   Démoulin, P.
2017shin.confE.160D    Altcode:
  Analyzing the transfer of magnetic helicity in active regions is a
  key component for understanding the nature of its coronal storage
  and release and for identifying its role in the coronal dynamics
  of active regions. We recently developed a method for studying the
  photospheric flux of magnetic helicity in both 2D and 3D. The method
  takes into account the 3D nature of magnetic helicity by explicitly
  using knowledge of the magnetic field connectivity. Since the coronal
  magnetic field in active regions is not measured, we rely on the
  approximate 3D solution obtained from force-free coronal magnetic
  field extrapolations to derive the magnetic field connectivity. In
  this poster, we apply the method to the complex and highly-flaring
  active region NOAA 11158 using the magnetic field connectivity derived
  from different force-free extrapolation models and implementations. We
  show that the calculations of photospheric flux of magnetic helicity
  are robust to different extrapolation methods and assumptions, in
  particular with regards to identifying regions of opposite magnetic
  helicity flux. Finally, we discuss the implications of our results
  for tracking the transfer of magnetic helicity in active regions and
  relate it to their flaring activity.

---------------------------------------------------------
Title: Measuring the magnetic field of a trans-equatorial loop system
    using coronal seismology
Authors: Long, D. M.; Valori, G.; Pérez-Suárez, D.; Morton, R. J.;
   Vásquez, A. M.
2017A&A...603A.101L    Altcode: 2017arXiv170310020L
  Context. EIT waves are freely-propagating global pulses in the low
  corona which are strongly associated with the initial evolution of
  coronal mass ejections (CMEs). They are thought to be large-amplitude,
  fast-mode magnetohydrodynamic waves initially driven by the rapid
  expansion of a CME in the low corona. <BR /> Aims: An EIT wave was
  observed on 6 July 2012 to impact an adjacent trans-equatorial loop
  system which then exhibited a decaying oscillation as it returned to
  rest. Observations of the loop oscillations were used to estimate the
  magnetic field strength of the loop system by studying the decaying
  oscillation of the loop, measuring the propagation of ubiquitous
  transverse waves in the loop and extrapolating the magnetic field
  from observed magnetograms. <BR /> Methods: Observations from the
  Atmospheric Imaging Assembly onboard the Solar Dynamics Observatory
  (SDO/AIA) and the Coronal Multi-channel Polarimeter (CoMP) were used
  to study the event. An Empirical Mode Decomposition analysis was used
  to characterise the oscillation of the loop system in CoMP Doppler
  velocity and line width and in AIA intensity. <BR /> Results: The
  loop system was shown to oscillate in the 2nd harmonic mode rather
  than at the fundamental frequency, with the seismological analysis
  returning an estimated magnetic field strength of ≈ 5.5 ± 1.5
  G. This compares to the magnetic field strength estimates of ≈1-9
  G and ≈3-9 G found using the measurements of transverse wave
  propagation and magnetic field extrapolation respectively. <P
  />A movie associated to Figs. 1 and 2 is available at <A
  href="http://www.aanda.org/10.1051/0004-6361/201730413/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: On-Disc Observations of Flux Rope Formation Prior to Its
    Eruption
Authors: James, A. W.; Green, L. M.; Palmerio, E.; Valori, G.; Reid,
   H. A. S.; Baker, D.; Brooks, D. H.; van Driel-Gesztelyi, L.; Kilpua,
   E. K. J.
2017SoPh..292...71J    Altcode: 2017arXiv170310837J
  Coronal mass ejections (CMEs) are one of the primary manifestations of
  solar activity and can drive severe space weather effects. Therefore,
  it is vital to work towards being able to predict their
  occurrence. However, many aspects of CME formation and eruption
  remain unclear, including whether magnetic flux ropes are present
  before the onset of eruption and the key mechanisms that cause CMEs
  to occur. In this work, the pre-eruptive coronal configuration of
  an active region that produced an interplanetary CME with a clear
  magnetic flux rope structure at 1 AU is studied. A forward-S sigmoid
  appears in extreme-ultraviolet (EUV) data two hours before the onset
  of the eruption (SOL2012-06-14), which is interpreted as a signature
  of a right-handed flux rope that formed prior to the eruption. Flare
  ribbons and EUV dimmings are used to infer the locations of the flux
  rope footpoints. These locations, together with observations of the
  global magnetic flux distribution, indicate that an interaction between
  newly emerged magnetic flux and pre-existing sunspot field in the days
  prior to the eruption may have enabled the coronal flux rope to form
  via tether-cutting-like reconnection. Composition analysis suggests
  that the flux rope had a coronal plasma composition, supporting our
  interpretation that the flux rope formed via magnetic reconnection in
  the corona. Once formed, the flux rope remained stable for two hours
  before erupting as a CME.

---------------------------------------------------------
Title: Analysis and modelling of recurrent solar flares observed
    with Hinode/EIS on March 9, 2012
Authors: Polito, V.; Del Zanna, G.; Valori, G.; Pariat, E.; Mason,
   H. E.; Dudík, J.; Janvier, M.
2017A&A...601A..39P    Altcode: 2016arXiv161203504P
  Three homologous C-class flares and one last M-class flare were observed
  by both the Solar Dynamics Observatory (SDO) and the Hinode EUV Imaging
  Spectrometer (EIS) in the AR 11429 on March 9, 2012. All the recurrent
  flares occurred within a short interval of time (less than 4 h),
  showed very similar plasma morphology and were all confined, until the
  last one when a large-scale eruption occurred. The C-class flares are
  characterized by the appearance, at approximatively the same locations,
  of two bright and compact footpoint sources of ≈3-10 MK evaporating
  plasma, and a semi-circular ribbon. During all the flares, the
  continuous brightening of a spine-like hot plasma (≈10 MK) structure
  is also observed. Spectroscopic observations with Hinode/EIS are used to
  measure and compare the blueshift velocities in the Fe xxiii emission
  line and the electron number density at the flare footpoints for each
  flare. Similar velocities, of the order of 150-200 km s<SUP>-1</SUP>,
  are observed during the C2.0 and C4.7 confined flares, in agreement
  with the values reported by other authors in the study of the last M1.8
  class flare. On the other hand, lower electron number densities and
  temperatures tend to be observed in flares with lower peak soft X-ray
  flux. In order to investigate the homologous nature of the flares, we
  performed a non-linear force-free field (NLFFF) extrapolation of the 3D
  magnetic field configuration in the corona. The NLFFF extrapolation and
  the Quasi-Separatrix Layers (QSLs) provide the magnetic field context
  which explains the location of the kernels, spine-like hot plasma and
  semi-circular brightenings observed in the (non-eruptive) flares. Given
  the absence of a coronal null point, we argue that the homologous
  flares were all generated by the continuous recurrence of bald patch
  reconnection. <P />The movie associated to Fig. 2 is available at <A
  href="http://www.aanda.org/10.1051/0004-6361/201629703/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: Relative magnetic helicity as a diagnostic of solar eruptivity
Authors: Pariat, E.; Leake, J. E.; Valori, G.; Linton, M. G.;
   Zuccarello, F. P.; Dalmasse, K.
2017A&A...601A.125P    Altcode: 2017arXiv170310562P
  Context. The discovery of clear criteria that can deterministically
  describe the eruptive state of a solar active region would lead
  to major improvements on space weather predictions. <BR /> Aims:
  Using series of numerical simulations of the emergence of a magnetic
  flux rope in a magnetized coronal, leading either to eruptions or to
  stable configurations, we test several global scalar quantities for
  the ability to discriminate between the eruptive and the non-eruptive
  simulations. <BR /> Methods: From the magnetic field generated by the
  three-dimensional magnetohydrodynamical simulations, we compute and
  analyze the evolution of the magnetic flux, of the magnetic energy
  and its decomposition into potential and free energies, and of the
  relative magnetic helicity and its decomposition. <BR /> Results:
  Unlike the magnetic flux and magnetic energies, magnetic helicities
  are able to markedly distinguish the eruptive from the non-eruptive
  simulations. We find that the ratio of the magnetic helicity of the
  current-carrying magnetic field to the total relative helicity presents
  the highest values for the eruptive simulations, in the pre-eruptive
  phase only. We observe that the eruptive simulations do not possess the
  highest value of total magnetic helicity. <BR /> Conclusions: In the
  framework of our numerical study, the magnetic energies and the total
  relative helicity do not correspond to good eruptivity proxies. Our
  study highlights that the ratio of magnetic helicities diagnoses very
  clearly the eruptive potential of our parametric simulations. Our study
  shows that magnetic-helicity-based quantities may be very efficient
  for the prediction of solar eruptions.

---------------------------------------------------------
Title: Magnetic Helicity Estimations in Models and Observations of
    the Solar Magnetic Field. III. Twist Number Method
Authors: Guo, Y.; Pariat, E.; Valori, G.; Anfinogentov, S.; Chen,
   F.; Georgoulis, M. K.; Liu, Y.; Moraitis, K.; Thalmann, J. K.; Yang, S.
2017ApJ...840...40G    Altcode: 2017arXiv170402096G
  We study the writhe, twist, and magnetic helicity of different
  magnetic flux ropes, based on models of the solar coronal magnetic
  field structure. These include an analytical force-free Titov-Démoulin
  equilibrium solution, non-force-free magnetohydrodynamic simulations,
  and nonlinear force-free magnetic field models. The geometrical
  boundary of the magnetic flux rope is determined by the quasi-separatrix
  layer and the bottom surface, and the axis curve of the flux rope is
  determined by its overall orientation. The twist is computed by the
  Berger-Prior formula, which is suitable for arbitrary geometry and
  both force-free and non-force-free models. The magnetic helicity is
  estimated by the twist multiplied by the square of the axial magnetic
  flux. We compare the obtained values with those derived by a finite
  volume helicity estimation method. We find that the magnetic helicity
  obtained with the twist method agrees with the helicity carried by the
  purely current-carrying part of the field within uncertainties for
  most test cases. It is also found that the current-carrying part of
  the model field is relatively significant at the very location of the
  magnetic flux rope. This qualitatively explains the agreement between
  the magnetic helicity computed by the twist method and the helicity
  contributed purely by the current-carrying magnetic field.

---------------------------------------------------------
Title: Magnetic helicity estimations in models and observations of
    the solar magnetic field
Authors: Valori, Gherardo; Pariat, Etienne; Anfinogentov, Sergey;
   Chen, Feng; Georgoulis, Manolis; Guo, Yang; Liu, Yang; Moraitis,
   Kostas; Thalmann, Julia K.; Yang, Shangbin
2017EGUGA..19.3692V    Altcode:
  Magnetic helicity, as one of the few conserved quantities
  in magneto-hydrodynamics, is often invoked as the principle
  driving the generation and structuring of magnetic fields in a
  variety of environments, from dynamo models in stars and planets,
  to post-disruption reconfigurations of tokamak's plasmas. Most
  particularly magnetic helicity has raised the interest of solar
  physicists, since helicity is suspected to represent a key quantity for
  the understanding of solar flares and the generation of coronal mass
  ejections. In recent years, several methods of estimation of magnetic
  helicity have been proposed and already applied to observations and
  numerical simulations. However, no systematic comparison of accuracy,
  mutual consistency, and reliability of such methods has ever been
  performed. We present the results of the first benchmark of several
  finite-volume methods in estimating magnetic helicity in 3D test
  models. In addition to finite volume methods, two additional methods
  are also included that estimate magnetic helicity based either on the
  field line's twist, or on the field's values on one boundary and an
  inferred minimal volume connectivity. The employed model tests range
  from solutions of the force-free equations to 3D magneto-hydrodynamical
  numerical simulations. Almost all methods are found to produce the same
  value of magnetic helicity within few percent in all tests. However,
  methods show differences in the sensitivity to numerical resolution and
  to errors in the solenoidal property of input fields. Our benchmark of
  finite volume methods allows to determine the reliability and precision
  of estimations of magnetic helicity in practical cases. As a next step,
  finite volume methods are used to test estimation methods that are
  based on the flux of helicity through one boundary, in particular
  for applications to observation-based models of coronal magnetic
  fields. The ultimate goal is to assess if and how can helicity be
  meaningfully used as a diagnostic of the evolution of magnetic fields
  in the solar atmosphere.

---------------------------------------------------------
Title: Determining the Intrinsic CME Flux Rope Type Using
    Remote-sensing Solar Disk Observations
Authors: Palmerio, E.; Kilpua, E. K. J.; James, A. W.; Green, L. M.;
   Pomoell, J.; Isavnin, A.; Valori, G.
2017SoPh..292...39P    Altcode: 2017arXiv170108595P
  A key aim in space weather research is to be able to use remote-sensing
  observations of the solar atmosphere to extend the lead time of
  predicting the geoeffectiveness of a coronal mass ejection (CME). In
  order to achieve this, the magnetic structure of the CME as it
  leaves the Sun must be known. In this article we address this issue
  by developing a method to determine the intrinsic flux rope type of
  a CME solely from solar disk observations. We use several well-known
  proxies for the magnetic helicity sign, the axis orientation, and the
  axial magnetic field direction to predict the magnetic structure of
  the interplanetary flux rope. We present two case studies: the 2 June
  2011 and the 14 June 2012 CMEs. Both of these events erupted from an
  active region, and despite having clear in situ counterparts, their
  eruption characteristics were relatively complex. The first event was
  associated with an active region filament that erupted in two stages,
  while for the other event the eruption originated from a relatively high
  coronal altitude and the source region did not feature a filament. Our
  magnetic helicity sign proxies include the analysis of magnetic
  tongues, soft X-ray and/or extreme-ultraviolet sigmoids, coronal
  arcade skew, filament emission and absorption threads, and filament
  rotation. Since the inclination of the post-eruption arcades was not
  clear, we use the tilt of the polarity inversion line to determine the
  flux rope axis orientation and coronal dimmings to determine the flux
  rope footpoints, and therefore, the direction of the axial magnetic
  field. The comparison of the estimated intrinsic flux rope structure
  to in situ observations at the Lagrangian point L1 indicated a good
  agreement with the predictions. Our results highlight the flux rope
  type determination techniques that are particularly useful for active
  region eruptions, where most geoeffective CMEs originate.

---------------------------------------------------------
Title: &lt;p&gt;Prediction of In-Situ Magnetic Structure of Flux
    Ropes from Coronal Observations.
Authors: Palmerio, E.; Kilpua, E.; James, A.; Green, L.; Pomoell,
   J.; Isavnin, A.; Valori, G.; Lumme, E.
2016AGUFMSH14A..03P    Altcode:
  Coronal mass ejections (CMEs) are believed to be the main drivers
  of intense magnetic storms and various space weather phenomena at
  Earth. The most important parameter that defines the ability of a
  CME to drive geomagnetic storms is the north-south magnetic field
  component. One of the most significant problems in current long-term
  space weather forecasts is that there is no method to directly
  measure the magnetic structure of CMEs before they are observed in
  situ. In recent years, CMEs have been successfully modeled as unstable
  expanding flux ropes originating from low-corona, force-free flux
  equilibria (either containing or forming a flux rope in the wake of the
  instability). Due to their influence on the coronal plasma environment,
  the magnetic structure of CME flux ropes can be indirectly estimated
  based on the properties of the source active region and characteristics
  of the nearby structures, such as filament details, coronal EUV arcades
  and X-ray sigmoids. We present here a study of two CME flux ropes,
  aiming at determining their magnetic properties (magnetic helicity
  sign, flux rope tilt, and direction of the flux rope axial field)
  when launched from the Sun by using a synthesis of indirect proxies
  based on multi-wavelength remote sensing observations. In addition,
  we employ a data-driven magnetofrictional method that models the CME
  initiation in the corona to determine the magnetic structure in the
  two case studies. Finally, the predictions given by the observational
  synthesis and coronal modeling are compared with the structure detected
  in situ at Earth.

---------------------------------------------------------
Title: Magnetic Helicity Estimations in Models and Observations of
the Solar Magnetic Field. Part I: Finite Volume Methods
Authors: Valori, Gherardo; Pariat, Etienne; Anfinogentov, Sergey;
   Chen, Feng; Georgoulis, Manolis K.; Guo, Yang; Liu, Yang; Moraitis,
   Kostas; Thalmann, Julia K.; Yang, Shangbin
2016SSRv..201..147V    Altcode: 2016SSRv..tmp...68V; 2016arXiv161002193V
  Magnetic helicity is a conserved quantity of ideal magneto-hydrodynamics
  characterized by an inverse turbulent cascade. Accordingly, it
  is often invoked as one of the basic physical quantities driving
  the generation and structuring of magnetic fields in a variety of
  astrophysical and laboratory plasmas. We provide here the first
  systematic comparison of six existing methods for the estimation of
  the helicity of magnetic fields known in a finite volume. All such
  methods are reviewed, benchmarked, and compared with each other,
  and specifically tested for accuracy and sensitivity to errors. To
  that purpose, we consider four groups of numerical tests, ranging
  from solutions of the three-dimensional, force-free equilibrium, to
  magneto-hydrodynamical numerical simulations. Almost all methods are
  found to produce the same value of magnetic helicity within few percent
  in all tests. In the more solar-relevant and realistic of the tests
  employed here, the simulation of an eruptive flux rope, the spread
  in the computed values obtained by all but one method is only 3 %,
  indicating the reliability and mutual consistency of such methods in
  appropriate parameter ranges. However, methods show differences in the
  sensitivity to numerical resolution and to errors in the solenoidal
  property of the input fields. In addition to finite volume methods,
  we also briefly discuss a method that estimates helicity from the
  field lines' twist, and one that exploits the field's value at one
  boundary and a coronal minimal connectivity instead of a pre-defined
  three-dimensional magnetic-field solution.

---------------------------------------------------------
Title: Measuring the magnetic field of a trans-equatorial loop system
    using coronal seismology
Authors: Long, David M.; Pérez-Suárez; D.; Valori; G.
2016usc..confE..25L    Altcode:
  First observed by SOHO/EIT, "EIT waves" are strongly associated with the
  initial evolution of coronal mass ejections (CMEs) and after almost 20
  years of investigation a consensus is being reached which interprets
  them as freely-propagating waves produced by the rapid expansion of
  a CME in the low corona. An "EIT wave" was observed on 6 July 2012
  to erupt from active region AR11514 into a particularly structured
  corona that included multiple adjacent active regions as well as an
  adjacent trans-equatorial loop system anchored at the boundary of a
  nearby coronal hole. The eruption was well observed by SDO/AIA and
  CoMP, allowing the effects of the "EIT wave" on the trans-equatorial
  loop system to be studied in detail. In particular, it was possible
  to characterise the oscillation of the loop system using Doppler
  velocity measurements from CoMP. These Doppler measurements were used
  to estimate the magnetic field strength of the trans-equatorial loop
  system via coronal seismology. It was then possible to compare these
  inferred magnetic field values with both extrapolated magnetic field
  values from a Potential Field Source Surface extrapolation as well
  as the direct measurements of magnetic field provided by CoMP. These
  results show that the magnetic field strength of loop systems in the
  solar corona may be estimated using loop seismology.

---------------------------------------------------------
Title: Prediction of in-situ magnetic structure of flux ropes from
    coronal observations
Authors: Palmerio, Erika; Kilpua, Emilia K. J.; Pomoell, Jens;
   James, Alexander; Green, Lucie M.; Isavnin, Alexey; Valori, Gherardo;
   Lumme, Erkka
2016usc..confE..33P    Altcode:
  Coronal Mass Ejections (CMEs) are built at the Sun as nearly force-free
  (J x B = 0) magnetic flux ropes. It is well-established that CMEs
  are the main drivers of intense magnetic storms and various space
  weather phenomena at Earth. The most important parameter that defines
  the ability of a CME to drive geomagnetic storms is the north-south
  magnetic field component. One of the most significant problems in
  current long-term space weather forecasts is that there is no method
  to directly measure the magnetic structure of CMEs before they are
  observed in situ. However, due to their influence on the coronal
  plasma environment, the magnetic structure of CME flux ropes can be
  indirectly estimated based on the properties of the source active
  region and characteristics of the nearby structures, such as filament
  details, coronal EUV arcades and X-ray sigmoids. We present here a
  study of two CME flux ropes, aiming at determining their magnetic
  properties (magnetic helicity sign, flux rope tilt, and direction
  of the flux rope axial field) when launched from the Sun by using a
  synthesis of indirect proxies based on multi-wavelength remote sensing
  observations. In addition, we employ a data-driven magnetofrictional
  method that models the CME initiation in the corona to determine the
  magnetic structure in the two case studies. Finally, the predictions
  given by the observational synthesis and coronal modeling are compared
  with the structure detected in situ at Earth.

---------------------------------------------------------
Title: Magneto-frictional Modeling of Coronal Nonlinear Force-free
    Fields. I. Testing with Analytic Solutions
Authors: Guo, Y.; Xia, C.; Keppens, R.; Valori, G.
2016ApJ...828...82G    Altcode:
  We report our implementation of the magneto-frictional method in the
  Message Passing Interface Adaptive Mesh Refinement Versatile Advection
  Code (MPI-AMRVAC). The method aims at applications where local adaptive
  mesh refinement (AMR) is essential to make follow-up dynamical modeling
  affordable. We quantify its performance in both domain-decomposed
  uniform grids and block-adaptive AMR computations, using all frequently
  employed force-free, divergence-free, and other vector comparison
  metrics. As test cases, we revisit the semi-analytic solution of Low
  and Lou in both Cartesian and spherical geometries, along with the
  topologically challenging Titov-Démoulin model. We compare different
  combinations of spatial and temporal discretizations, and find that the
  fourth-order central difference with a local Lax-Friedrichs dissipation
  term in a single-step marching scheme is an optimal combination. The
  initial condition is provided by the potential field, which is the
  potential field source surface model in spherical geometry. Various
  boundary conditions are adopted, ranging from fully prescribed cases
  where all boundaries are assigned with the semi-analytic models,
  to solar-like cases where only the magnetic field at the bottom is
  known. Our results demonstrate that all the metrics compare favorably
  to previous works in both Cartesian and spherical coordinates. Cases
  with several AMR levels perform in accordance with their effective
  resolutions. The magneto-frictional method in MPI-AMRVAC allows us
  to model a region of interest with high spatial resolution and large
  field of view simultaneously, as required by observation-constrained
  extrapolations using vector data provided with modern instruments. The
  applications of the magneto-frictional method to observations are
  shown in an accompanying paper.

---------------------------------------------------------
Title: Flux Cancellation and the Evolution of the Eruptive Filament
    of 2011 June 7
Authors: Yardley, S. L.; Green, L. M.; Williams, D. R.; van
   Driel-Gesztelyi, L.; Valori, G.; Dacie, S.
2016ApJ...827..151Y    Altcode: 2016arXiv160608264Y
  We investigate whether flux cancellation is responsible for the
  formation of a very massive filament resulting in the spectacular
  eruption on 2011 June 7. We analyze and quantify the amount of flux
  cancellation that occurs in NOAA AR 11226 and its two neighboring active
  regions (ARs 11227 &amp; 11233) using line-of-sight magnetograms from
  the Heliospheric Magnetic Imager. During a 3.6 day period building
  up to the eruption of the filament, 1.7 × 10<SUP>21</SUP> Mx, 21%
  of AR 11226's maximum magnetic flux, was canceled along the polarity
  inversion line (PIL) where the filament formed. If the flux cancellation
  continued at the same rate up until the eruption then up to 2.8 ×
  10<SUP>21</SUP> Mx (34% of the AR flux) may have been built into the
  magnetic configuration that contains the filament plasma. The large flux
  cancellation rate is due to an unusual motion of the positive-polarity
  sunspot, which splits, with the largest section moving rapidly toward
  the PIL. This motion compresses the negative polarity and leads to
  the formation of an orphan penumbra where one end of the filament is
  rooted. Dense plasma threads above the orphan penumbra build into the
  filament, extending its length, and presumably injecting material into
  it. We conclude that the exceptionally strong flux cancellation in
  AR 11226 played a significant role in the formation of its unusually
  massive filament. In addition, the presence and coherent evolution of
  bald patches in the vector magnetic field along the PIL suggest that
  the magnetic field configuration supporting the filament material is
  that of a flux rope.

---------------------------------------------------------
Title: Photospheric Vector Magnetic Field Evolution of NOAA Active
    Region 11504 and the Ensuing CME
Authors: James, Alexander; Green, Lucie; Valori, Gherardo; van
   Driel-Gesztelyi, Lidia; Baker, Deborah; Brooks, David; Palmerio, Erika
2016SPD....4730305J    Altcode:
  Coronal mass ejections (CMEs) are eruptions of billions of tonnes of
  plasma from the Sun that drive the most severe space weather effects
  we observe. In order to be able to produce forecasts of space weather
  with lead times of the order of days, accurate predictions of the
  occurrence of CMEs must be developed. The eruptive active-region
  studied in this work (NOAA 11504) is complex, featuring fragmentation
  of penumbral magnetic field in the days prior to eruption, as well as
  rotation of the leading sunspot. SDO/HMI vector photospheric magnetic
  field measurements are utilised alongside SDO/AIA multi-wavelength
  extreme ultra-violet (EUV) observations to study the dynamics of the
  photospheric and coronal structures, as well as Hinode/EIS spectroscopic
  measurements, including elemental composition data. The EUV data show
  flare ribbons as well as coronal dimmings, which are used to infer
  the orientation of the erupting flux rope. This flux rope orientation
  is then compared to in situ measurements of the flux rope. The vector
  magnetic field data is used to determine the possible contributions
  the field fragmentation and sunspot rotation may have made to the
  formation of the flux rope and the triggering of the CME.

---------------------------------------------------------
Title: Measuring the magnetic field of a trans-equatorial loop system
    using coronal seismology
Authors: Long, David; Perez-Suarez, David; Valori, Gherardo
2016SPD....47.0319L    Altcode:
  First observed by SOHO/EIT, "EIT waves" are strongly associated with the
  initial evolution of coronal mass ejections (CMEs) and after almost 20
  years of investigation a consensus is being reached which interprets
  them as freely-propagating waves produced by the rapid expansion of
  a CME in the low corona. An "EIT wave" was observed on 6 July 2012
  to erupt from active region AR11514 into a particularly structured
  corona that included multiple adjacent active regions as well as an
  adjacent trans-equatorial loop system anchored at the boundary of a
  nearby coronal hole. The eruption was well observed by SDO/AIA and
  CoMP, allowing the effects of the "EIT wave" on the trans-equatorial
  loop system to be studied in detail. In particular, it was possible
  to characterise the oscillation of the loop system using Doppler
  velocity measurements from CoMP. These Doppler measurements were used
  to estimate the magnetic field strength of the trans-equatorial loop
  system via coronal seismology. It was then possible to compare these
  inferred magnetic field values with extrapolated magnetic field values
  derived using a Potential Field Source Surface extrapolation as well
  as the direct measurements of magnetic field provided by CoMP. These
  results show that the magnetic field strength of loop systems in the
  solar corona may be estimated using loop seismology.

---------------------------------------------------------
Title: Anomalous transmission of a coronal "EIT wave" through a
    nearby coronal hole
Authors: Long, David; Perez-Suarez, David; Valori, Gherardo
2016SPD....47.0320L    Altcode:
  Observations of reflection at coronal hole boundaries and transmission
  through the coronal hole suggest that "EIT waves" may be interpreted
  as freely--propagating wave--pulses initially driven by the rapid
  expansion of a coronal mass ejection (CME) in the low corona. An
  "EIT wave" observed on 2012 July 07 is seen to impact an adjacent
  coronal hole. However, rather than reappearing at the far edge of
  the coronal hole as with previous observations, the "EIT wave" was
  subsequently observed to reappear ~360 Mm away in the quiet Sun. The
  non-typical evolution of the "EIT wave" is examined using a combination
  of observations of the eruption from SDO/AIA and STEREO-A/EUVI as well
  as extrapolations of the global magnetic field. The observed "jump"
  in position of the "EIT wave" is shown to be due to the wave pulse
  traveling along hot coronal loops connecting the edge of the coronal
  hole with the quiet Sun.

---------------------------------------------------------
Title: Tracking the magnetic structure of flux ropes from eruption
    to in-situ detection
Authors: Palmerio, Erika; Kilpua, Emilia; Green, Lucie; James,
   Alexander; Pomoell, Jens; Valori, Gherardo
2016EGUGA..18.1641P    Altcode:
  Coronal Mass Ejections (CMEs) are spectacular explosions from the
  Sun where huge amounts of plasma and magnetic flux are ejected into
  the heliosphere. CMEs are built at the Sun as a force-free (J ×B =
  0) magnetic flux rope. It is well-established that CMEs are the main
  drivers of intense magnetic storms and various space weather effects
  at the Earth. One of the most significant problems for improving the
  long lead-time space weather predictions is that there is no method to
  directly measure the structure of CME magnetic fields, neither in the
  onset process nor during the subsequent propagation from the solar
  surface to the Earth. The magnetic properties of the CME flux rope
  (magnetic helicity sign, the flux rope tilt and the direction of the
  flux rope axial field) can be estimated based on the properties of the
  source active region and characteristics of the related structures, such
  as filament details, coronal EUV arcades and X-ray sigmoids. We present
  here a study of two CME flux ropes. We compare their magnetic structure
  using the synthesis of these indirect proxies based on multi-wavelength
  remote sensing observations with the structure detected in-situ near
  the orbit of the Earth.

---------------------------------------------------------
Title: Restricted propagation of an “EIT wave” in the low solar
    corona
Authors: Long, David M.; Pérez-Suárez, David; Valori, Gherardo
2016IAUS..320...98L    Altcode:
  We present observations of an “EIT wave” associated with an X-class
  flare from 2012 July 6, the propagation of which was severely restricted
  by the magnetic structure of the solar corona surrounding the erupting
  active region. The “EIT wave” was observed by both SDO and STEREO-A,
  allowing a three-dimensional examination of how the propagation of
  the disturbance was affected both by a neighbouring coronal hole
  and a trans-equatorial loop system. In addition, the eruption was
  observed at the limb by the ground-based CoMP instrument, allowing the
  Doppler motion associated with the eruption and resulting coronal loop
  oscillation to be investigated in detail. This combination of data-sets
  provides a unique insight into the three-dimensional evolution of the
  “EIT wave” and its effects on the surrounding corona.

---------------------------------------------------------
Title: The Influence of Spatial resolution on Nonlinear Force-free
    Modeling
Authors: DeRosa, M. L.; Wheatland, M. S.; Leka, K. D.; Barnes, G.;
   Amari, T.; Canou, A.; Gilchrist, S. A.; Thalmann, J. K.; Valori,
   G.; Wiegelmann, T.; Schrijver, C. J.; Malanushenko, A.; Sun, X.;
   Régnier, S.
2015ApJ...811..107D    Altcode: 2015arXiv150805455D
  The nonlinear force-free field (NLFFF) model is often used to
  describe the solar coronal magnetic field, however a series of
  earlier studies revealed difficulties in the numerical solution of the
  model in application to photospheric boundary data. We investigate
  the sensitivity of the modeling to the spatial resolution of the
  boundary data, by applying multiple codes that numerically solve the
  NLFFF model to a sequence of vector magnetogram data at different
  resolutions, prepared from a single Hinode/Solar Optical Telescope
  Spectro-Polarimeter scan of NOAA Active Region 10978 on 2007 December
  13. We analyze the resulting energies and relative magnetic helicities,
  employ a Helmholtz decomposition to characterize divergence errors, and
  quantify changes made by the codes to the vector magnetogram boundary
  data in order to be compatible with the force-free model. This study
  shows that NLFFF modeling results depend quantitatively on the spatial
  resolution of the input boundary data, and that using more highly
  resolved boundary data yields more self-consistent results. The
  free energies of the resulting solutions generally trend higher
  with increasing resolution, while relative magnetic helicity values
  vary significantly between resolutions for all methods. All methods
  require changing the horizontal components, and for some methods also
  the vertical components, of the vector magnetogram boundary field in
  excess of nominal uncertainties in the data. The solutions produced
  by the various methods are significantly different at each resolution
  level. We continue to recommend verifying agreement between the modeled
  field lines and corresponding coronal loop images before any NLFFF
  model is used in a scientific setting.

---------------------------------------------------------
Title: Testing magnetic helicity conservation in a solar-like
    active event
Authors: Pariat, E.; Valori, G.; Démoulin, P.; Dalmasse, K.
2015A&A...580A.128P    Altcode: 2015arXiv150609013P
  Context. Magnetic helicity has the remarkable property of being a
  conserved quantity of ideal magnetohydrodynamics (MHD). Therefore, it
  could be used as an effective tracer of the magnetic field evolution
  of magnetized plasmas. <BR /> Aims: Theoretical estimations indicate
  that magnetic helicity is also essentially conserved with non-ideal MHD
  processes, for example, magnetic reconnection. This conjecture has been
  barely tested, however, either experimentally or numerically. Thanks
  to recent advances in magnetic helicity estimation methods, it is
  now possible to numerically test its dissipation level in general
  three-dimensional datasets. <BR /> Methods: We first revisit the
  general formulation of the temporal variation of relative magnetic
  helicity on a fully bounded volume when no hypothesis on the gauge is
  made. We introduce a method for precisely estimating its dissipation
  independently of which type of non-ideal MHD processes occurs. For
  a solar-like eruptive-event simulation, using different gauges, we
  compare an estimate of the relative magnetic helicity computed in a
  finite volume with its time-integrated flux through the boundaries. We
  thus test the conservation and dissipation of helicity. <BR /> Results:
  We provide an upper bound of the real dissipation of magnetic helicity:
  It is quasi-null during the quasi-ideal MHD phase. Even with magnetic
  reconnection, the relative dissipation of magnetic helicity is also very
  low (&lt;2.2%), in particular compared to the relative dissipation
  of magnetic energy (&gt;30 times higher). We finally illustrate
  how the helicity-flux terms involving velocity components are gauge
  dependent, which limits their physical meaning. <BR /> Conclusions:
  Our study paves the way for more extended and diverse tests of the
  magnetic helicity conservation properties. Our study confirms the
  central role of helicity in the study of MHD plasmas. For instance,
  the conservation of helicity can be used to track the evolution of
  solar magnetic fields from when they form in the solar interior
  until their detection as magnetic clouds in the interplanetary
  space. <P />Appendix A is available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201525811/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: Time Evolution of Force-Free Parameter and Free Magnetic
    Energy in Active Region NOAA 10365
Authors: Valori, G.; Romano, P.; Malanushenko, A.; Ermolli, I.;
   Giorgi, F.; Steed, K.; van Driel-Gesztelyi, L.; Zuccarello, F.;
   Malherbe, J. -M.
2015SoPh..290..491V    Altcode:
  We describe the variation of the accumulated coronal helicity derived
  from the magnetic helicity flux through the photosphere in active region
  (AR) NOAA 10365, where several large flares and coronal mass ejections
  (CMEs) occurred. We used SOHO/MDI full-disk line-of-sight magnetograms
  to measure the helicity flux, and the integral of GOES X-ray flux as a
  proxy of the coronal energy variations due to flares or CMEs. Using the
  linear force-free field model, we transformed the accumulated helicity
  flux into a time sequence of the force-free parameter α accounting for
  flares or CMEs via the proxy derived from GOES observations. This method
  can be used to derive the value of α at different times during the
  AR evolution, and is a partial alternative to the commonly used match
  of field lines with EUV loops. By combining the accumulated helicity
  obtained from the observations with the linear force-free theory, we
  describe the main phases of the emergence process of the AR, and relate
  them temporally with the occurrence of flares or CMEs. Additionally,
  a comparison with the loop-matching method of fixing alpha at each time
  independently shows that the proposed method may be helpful in avoiding
  unrealistic or undetermined values of alpha that may originate from
  an insufficient quality of the image used to identify coronal loops
  at a given time. For the relative intensity of the considered events,
  the linear force-free field theory implies that there is a direct
  correlation between the released energy on the one hand and the product
  of the coronal helicity with the variation of α due to the event on
  the other. Therefore, the higher the value of the accumulated coronal
  helicity, the smaller the force-free parameter variation required to
  produce the same decrease in the free energy during the CMEs.

---------------------------------------------------------
Title: Coronal Magnetic Reconnection Driven by CME Expansion—the
    2011 June 7 Event
Authors: van Driel-Gesztelyi, L.; Baker, D.; Török, T.; Pariat, E.;
   Green, L. M.; Williams, D. R.; Carlyle, J.; Valori, G.; Démoulin,
   P.; Kliem, B.; Long, D. M.; Matthews, S. A.; Malherbe, J. -M.
2014ApJ...788...85V    Altcode: 2014arXiv1406.3153V
  Coronal mass ejections (CMEs) erupt and expand in a magnetically
  structured solar corona. Various indirect observational pieces of
  evidence have shown that the magnetic field of CMEs reconnects with
  surrounding magnetic fields, forming, e.g., dimming regions distant
  from the CME source regions. Analyzing Solar Dynamics Observatory
  (SDO) observations of the eruption from AR 11226 on 2011 June 7, we
  present the first direct evidence of coronal magnetic reconnection
  between the fields of two adjacent active regions during a CME. The
  observations are presented jointly with a data-constrained numerical
  simulation, demonstrating the formation/intensification of current
  sheets along a hyperbolic flux tube at the interface between the CME
  and the neighboring AR 11227. Reconnection resulted in the formation of
  new magnetic connections between the erupting magnetic structure from
  AR 11226 and the neighboring active region AR 11227 about 200 Mm from
  the eruption site. The onset of reconnection first becomes apparent
  in the SDO/AIA images when filament plasma, originally contained
  within the erupting flux rope, is redirected toward remote areas in
  AR 11227, tracing the change of large-scale magnetic connectivity. The
  location of the coronal reconnection region becomes bright and directly
  observable at SDO/AIA wavelengths, owing to the presence of down-flowing
  cool, dense (10<SUP>10</SUP> cm<SUP>-3</SUP>) filament plasma in its
  vicinity. The high-density plasma around the reconnection region is
  heated to coronal temperatures, presumably by slow-mode shocks and
  Coulomb collisions. These results provide the first direct observational
  evidence that CMEs reconnect with surrounding magnetic structures,
  leading to a large-scale reconfiguration of the coronal magnetic field.

---------------------------------------------------------
Title: Constraining magnetic flux emergence from a timeseries of
    helicitigrams
Authors: Dalmasse, Kévin; Pariat, Etienne; Green, Lucie M.; Aulanier,
   Guillaume; Demoulin, Pascal; Valori, Gherardo
2014cosp...40E.612D    Altcode:
  Magnetic helicity quantifies how globally twisted and/or sheared is
  the magnetic field in a volume. Observational studies have reported
  the injection of large amounts of magnetic helicity associated with
  the emergence of magnetic flux into the solar atmosphere. Because
  magnetic helicity is conserved in the convection zone, the injection of
  magnetic helicity into the solar corona reflects the helicity content
  of emerging magnetic flux tubes. Mapping the photospheric injection
  of magnetic helicity thus seems to be a key tool for constraining the
  parameters of the emerging flux tubes in numerical case-studies of
  observed active regions. We recently developed a method to compute the
  distribution of magnetic helicity flux. Contrary to previous proxies,
  this method takes into account the 3D nature of magnetic helicity, and
  is thus, better-suited to study the distribution of helicity flux. After
  introducing this method, we will present the results of its application
  to the NOAA AR 11158. We will show that, the distribution of helicity
  flux is complex, with patterns of real mixed signals of helicity flux
  related to the specific topology of the active region's magnetic
  field. Finally, we will discuss the implications of our results on
  the evolution and dynamics of this active region.

---------------------------------------------------------
Title: Magnetic reconnection driven by filament eruption in the 7
    June 2011 event
Authors: van Driel-Gesztelyi, L.; Baker, D.; Török, T.; Pariat, E.;
   Green, L. M.; Williams, D. R.; Carlyle, J.; Valori, G.; Démoulin,
   P.; Matthews, S. A.; Kliem, B.; Malherbe, J. -M.
2014IAUS..300..502V    Altcode:
  During an unusually massive filament eruption on 7 June 2011,
  SDO/AIA imaged for the first time significant EUV emission around a
  magnetic reconnection region in the solar corona. The reconnection
  occurred between magnetic fields of the laterally expanding CME
  and a neighbouring active region. A pre-existing quasi-separatrix
  layer was activated in the process. This scenario is supported by
  data-constrained numerical simulations of the eruption. Observations
  show that dense cool filament plasma was re-directed and heated in
  situ, producing coronal-temperature emission around the reconnection
  region. These results provide the first direct observational evidence,
  supported by MHD simulations and magnetic modelling, that a large-scale
  re-configuration of the coronal magnetic field takes place during
  solar eruptions via the process of magnetic reconnection.

---------------------------------------------------------
Title: Initiation of Coronal Mass Ejections by Sunspot Rotation
Authors: Valori, G.; Török, T.; Temmer, M.; Veronig, A. M.; van
   Driel-Gesztelyi, L.; Vršnak, B.
2014IAUS..300..201V    Altcode:
  We report observations of a filament eruption, two-ribbon flare, and
  coronal mass ejection (CME) that occurred in Active Region NOAA 10898
  on 6 July 2006. The filament was located South of a strong sunspot that
  dominated the region. In the evolution leading up to the eruption, and
  for some time after it, a counter-clockwise rotation of the sunspot of
  about 30 degrees was observed. We suggest that the rotation triggered
  the eruption by progressively expanding the magnetic field above the
  filament. To test this scenario, we study the effect of twisting
  the initially potential field overlying a pre-existing flux rope,
  using three-dimensional zero-β MHD simulations. We consider a magnetic
  configuration whose photospheric flux distribution and coronal structure
  is guided by the observations and a potential field extrapolation. We
  find that the twisting leads to the expansion of the overlying field. As
  a consequence of the progressively reduced magnetic tension, the flux
  rope quasi-statically adapts to the changed environmental field, rising
  slowly. Once the tension is sufficiently reduced, a distinct second
  phase of evolution occurs where the flux rope enters an unstable regime
  characterized by a strong acceleration. Our simulation thus suggests
  a new mechanism for the triggering of eruptions in the vicinity of
  rotating sunspots.

---------------------------------------------------------
Title: Initiation of Coronal Mass Ejections by Sunspot Rotation
Authors: Török, T.; Temmer, M.; Valori, G.; Veronig, A. M.; van
   Driel-Gesztelyi, L.; Vršnak, B.
2013SoPh..286..453T    Altcode: 2014arXiv1401.2922T
  We study a filament eruption, two-ribbon flare, and coronal mass
  ejection (CME) that occurred in NOAA Active Region 10898 on 6 July
  2006. The filament was located South of a strong sunspot that dominated
  the region. In the evolution leading up to the eruption, and for some
  time after it, a counter-clockwise rotation of the sunspot of about
  30 degrees was observed. We suggest that the rotation triggered the
  eruption by progressively expanding the magnetic field above the
  filament. To test this scenario, we study the effect of twisting
  the initially potential field overlying a pre-existing flux-rope,
  using three-dimensional zero-β MHD simulations. We first consider
  a relatively simple and symmetric system, and then study a more
  complex and asymmetric magnetic configuration, whose photospheric-flux
  distribution and coronal structure are guided by the observations and a
  potential field extrapolation. In both cases, we find that the twisting
  leads to the expansion of the overlying field. As a consequence of the
  progressively reduced magnetic tension, the flux-rope quasi-statically
  adapts to the changed environmental field, rising slowly. Once the
  tension is sufficiently reduced, a distinct second phase of evolution
  occurs where the flux-rope enters an unstable regime characterised by
  a strong acceleration. Our simulations thus suggest a new mechanism
  for the triggering of eruptions in the vicinity of rotating sunspots.

---------------------------------------------------------
Title: First observational application of a connectivity-based
    helicity flux density
Authors: Dalmasse, K.; Pariat, E.; Valori, G.; Démoulin, P.; Green,
   L. M.
2013A&A...555L...6D    Altcode: 2013arXiv1307.2838D
  Context. Measuring the magnetic helicity distribution in the solar
  corona can help in understanding the trigger of solar eruptive
  events because magnetic helicity is believed to play a key role in
  solar activity due to its conservation property. <BR /> Aims: A new
  method for computing the photospheric distribution of the helicity
  flux was recently developed. This method takes into account the
  magnetic field connectivity whereas previous methods were based
  on photospheric signatures only. This novel method maps the true
  injection of magnetic helicity in active regions. We applied this
  method for the first time to an observed active region, NOAA 11158,
  which was the source of intense flaring activity. <BR /> Methods: We
  used high-resolution vector magnetograms from the SDO/HMI instrument
  to compute the photospheric flux transport velocities and to perform
  a nonlinear force-free magnetic field extrapolation. We determined
  and compared the magnetic helicity flux distribution using a purely
  photospheric as well as a connectivity-based method. <BR /> Results:
  While the new connectivity-based method confirms the mixed pattern
  of the helicity flux in NOAA 11158, it also reveals a different, and
  more correct, distribution of the helicity injection. This distribution
  can be important for explaining the likelihood of an eruption from the
  active region. <BR /> Conclusions: The connectivity-based approach is
  a robust method for computing the magnetic helicity flux, which can
  be used to study the link between magnetic helicity and eruptivity of
  observed active regions.

---------------------------------------------------------
Title: Accuracy of magnetic energy computations
Authors: Valori, G.; Démoulin, P.; Pariat, E.; Masson, S.
2013A&A...553A..38V    Altcode: 2013arXiv1303.6773V
  Context. For magnetically driven events, the magnetic energy of
  the system is the prime energy reservoir that fuels the dynamical
  evolution. In the solar context, the free energy (i.e., the energy in
  excess of the potential field energy) is one of the main indicators
  used in space weather forecasts to predict the eruptivity of active
  regions. A trustworthy estimation of the magnetic energy is therefore
  needed in three-dimensional (3D) models of the solar atmosphere, e.g.,
  in coronal fields reconstructions or numerical simulations. <BR /> Aims:
  The expression of the energy of a system as the sum of its potential
  energy and its free energy (Thomson's theorem) is strictly valid when
  the magnetic field is exactly solenoidal. For numerical realizations on
  a discrete grid, this property may be only approximately fulfilled. We
  show that the imperfect solenoidality induces terms in the energy that
  can lead to misinterpreting the amount of free energy present in a
  magnetic configuration. <BR /> Methods: We consider a decomposition
  of the energy in solenoidal and nonsolenoidal parts which allows
  the unambiguous estimation of the nonsolenoidal contribution to the
  energy. We apply this decomposition to six typical cases broadly used
  in solar physics. We quantify to what extent the Thomson theorem is
  not satisfied when approximately solenoidal fields are used. <BR />
  Results: The quantified errors on energy vary from negligible to
  significant errors, depending on the extent of the nonsolenoidal
  component of the field. We identify the main source of errors and
  analyze the implications of adding a variable amount of divergence to
  various solenoidal fields. Finally, we present pathological unphysical
  situations where the estimated free energy would appear to be negative,
  as found in some previous works, and we identify the source of this
  error to be the presence of a finite divergence. <BR /> Conclusions:
  We provide a method of quantifying the effect of a finite divergence in
  numerical fields, together with detailed diagnostics of its sources. We
  also compare the efficiency of two divergence-cleaning techniques. These
  results are applicable to a broad range of numerical realizations of
  magnetic fields. <P />Appendices are available in electronic form at
  <A href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: Comparing Values of the Relative Magnetic Helicity in Finite
    Volumes
Authors: Valori, G.; Démoulin, P.; Pariat, E.
2012SoPh..278..347V    Altcode: 2012SoPh..tmp..271G
  Relative magnetic helicity, as a conserved quantity of ideal
  magnetohydrodynamics, has been highlighted as an important quantity to
  study in plasma physics. Due to its nonlocal nature, its estimation
  is not straightforward in both observational and numerical data. In
  this study we derive expressions for the practical computation of the
  gauge-independent relative magnetic helicity in three-dimensional
  finite domains. The derived expressions are easy to implement and
  rapid to compute. They are derived in Cartesian coordinates, but can
  be easily written in other coordinate systems. We apply our method to
  a numerical model of a force-free equilibrium containing a flux rope,
  and compare the results with those obtained employing known half-space
  equations. We find that our method requires a much smaller volume
  than half-space expressions to derive the full helicity content. We
  also prove that values of relative magnetic helicity of different
  magnetic fields can be compared with each other in the same sense as
  free-energy values can. Therefore, relative magnetic helicity can
  be meaningfully and directly compared between different datasets,
  such as those from different active regions, but also within the
  same dataset at different times. Typical applications of our formulae
  include the helicity computation in three-dimensional models of the
  solar atmosphere, e.g., coronal-field reconstructions by force-free
  extrapolation and discretized magnetic fields of numerical simulations.

---------------------------------------------------------
Title: Nonlinear Force-Free Extrapolation of Emerging Flux with a
    Global Twist and Serpentine Fine Structures
Authors: Valori, G.; Green, L. M.; Démoulin, P.; Vargas Domínguez,
   S.; van Driel-Gesztelyi, L.; Wallace, A.; Baker, D.; Fuhrmann, M.
2012SoPh..278...73V    Altcode:
  We study the flux emergence process in NOAA active region 11024, between
  29 June and 7 July 2009, by means of multi-wavelength observations
  and nonlinear force-free extrapolation. The main aim is to extend
  previous investigations by combining, as much as possible, high spatial
  resolution observations to test our present understanding of small-scale
  (undulatory) flux emergence, whilst putting these small-scale events
  in the context of the global evolution of the active region. The
  combination of these techniques allows us to follow the whole process,
  from the first appearance of the bipolar axial field on the east limb,
  until the buoyancy instability could set in and raise the main body
  of the twisted flux tube through the photosphere, forming magnetic
  tongues and signatures of serpentine field, until the simplification
  of the magnetic structure into a main bipole by the time the active
  region reaches the west limb. At the crucial time of the main emergence
  phase high spatial resolution spectropolarimetric measurements of the
  photospheric field are employed to reconstruct the three-dimensional
  structure of the nonlinear force-free coronal field, which is then
  used to test the current understanding of flux emergence processes. In
  particular, knowledge of the coronal connectivity confirms the identity
  of the magnetic tongues as seen in their photospheric signatures,
  and it exemplifies how the twisted flux, which is emerging on small
  scales in the form of a sea-serpent, is subsequently rearranged by
  reconnection into the large-scale field of the active region. In
  this way, the multi-wavelength observations combined with a nonlinear
  force-free extrapolation provide a coherent picture of the emergence
  process of small-scale magnetic bipoles, which subsequently reconnect
  to form a large-scale structure in the corona.

---------------------------------------------------------
Title: A comparison of preprocessing methods for solar force-free
    magnetic field extrapolation
Authors: Fuhrmann, M.; Seehafer, N.; Valori, G.; Wiegelmann, T.
2011A&A...526A..70F    Altcode: 2010arXiv1010.6015F
  Context. Extrapolations of solar photospheric vector magnetograms into
  three-dimensional magnetic fields in the chromosphere and corona are
  usually done under the assumption that the fields are force-free. This
  condition is violated in the photosphere itself and a thin layer in
  the lower atmosphere above. The field calculations can be improved
  by preprocessing the photospheric magnetograms. The intention here
  is to remove a non-force-free component from the data. <BR /> Aims:
  We compare two preprocessing methods presently in use, namely the
  methods of Wiegelmann et al. (2006, Sol. Phys., 233, 215) and Fuhrmann
  et al. (2007, A&amp;A, 476, 349). <BR /> Methods: The two preprocessing
  methods were applied to a vector magnetogram of the recently observed
  active region NOAA AR 10 953. We examine the changes in the magnetogram
  effected by the two preprocessing algorithms. Furthermore, the original
  magnetogram and the two preprocessed magnetograms were each used as
  input data for nonlinear force-free field extrapolations by means of two
  different methods, and we analyze the resulting fields. <BR /> Results:
  Both preprocessing methods managed to significantly decrease the
  magnetic forces and magnetic torques that act through the magnetogram
  area and that can cause incompatibilities with the assumption of
  force-freeness in the solution domain. The force and torque decrease is
  stronger for the Fuhrmann et al. method. Both methods also reduced the
  amount of small-scale irregularities in the observed photospheric field,
  which can sharply worsen the quality of the solutions. For the chosen
  parameter set, the Wiegelmann et al. method led to greater changes
  in strong-field areas, leaving weak-field areas mostly unchanged,
  and thus providing an approximation of the magnetic field vector in
  the chromosphere, while the Fuhrmann et al. method weakly changed
  the whole magnetogram, thereby better preserving patterns present
  in the original magnetogram. Both preprocessing methods raised the
  magnetic energy content of the extrapolated fields to values above the
  minimum energy, corresponding to the potential field. Also, the fields
  calculated from the preprocessed magnetograms fulfill the solenoidal
  condition better than those calculated without preprocessing.

---------------------------------------------------------
Title: Testing magnetofrictional extrapolation with the
    Titov-Démoulin model of solar active regions
Authors: Valori, G.; Kliem, B.; Török, T.; Titov, V. S.
2010A&A...519A..44V    Altcode: 2010arXiv1005.0254V
  We examine the nonlinear magnetofrictional extrapolation scheme
  using the solar active region model by Titov and Démoulin as test
  field. This model consists of an arched, line-tied current channel
  held in force-free equilibrium by the potential field of a bipolar
  flux distribution in the bottom boundary. A modified version with a
  parabolic current density profile is employed here. We find that the
  equilibrium is reconstructed with very high accuracy in a representative
  range of parameter space, using only the vector field in the bottom
  boundary as input. Structural features formed in the interface
  between the flux rope and the surrounding arcade - “hyperbolic
  flux tube” and “bald patch separatrix surface” - are reliably
  reproduced, as are the flux rope twist and the energy and helicity of
  the configuration. This demonstrates that force-free fields containing
  these basic structural elements of solar active regions can be obtained
  by extrapolation. The influence of the chosen initial condition on
  the accuracy of reconstruction is also addressed, confirming that the
  initial field that best matches the external potential field of the
  model quite naturally leads to the best reconstruction. Extrapolating
  the magnetogram of a Titov-Démoulin equilibrium in the unstable
  range of parameter space yields a sequence of two opposing evolutionary
  phases, which clearly indicate the unstable nature of the configuration:
  a partial buildup of the flux rope with rising free energy is followed
  by destruction of the rope, losing most of the free energy.

---------------------------------------------------------
Title: Nonlinear Force-Free Magnetic Field Modeling of AR 10953:
    A Critical Assessment
Authors: De Rosa, Marc L.; Schrijver, C. J.; Barnes, G.; Leka, K. D.;
   Lites, B. W.; Aschwanden, M. J.; Amari, T.; Canou, A.; McTiernan,
   J. M.; Régnier, S.; Thalmann, J. K.; Valori, G.; Wheatland, M. S.;
   Wiegelmann, T.; Cheung, M. C. M.; Conlon, P. A.; Fuhrmann, M.;
   Inhester, B.; Tadesse, T.
2009SPD....40.3102D    Altcode:
  Nonlinear force-free field (NLFFF) modeling seeks to provide accurate
  representations of the structure of the magnetic field above solar
  active regions, from which estimates of physical quantities of interest
  (e.g., free energy and helicity) can be made. However, the suite of
  NLFFF algorithms have failed to arrive at consistent solutions when
  applied to (thus far, two) cases using the highest-available-resolution
  vector magnetogram data from Hinode/SOT-SP (in the region of the
  modeling area of interest) and line-of-sight magnetograms from
  SOHO/MDI (where vector data were not available). One issue is that
  NLFFF models require consistent, force-free vector magnetic boundary
  data, and vector magnetogram data sampling the photosphere do not
  satisfy this requirement. Consequently, several problems have arisen
  that are believed to affect such modeling efforts. We use AR 10953
  to illustrate these problems, namely: (1) some of the far-reaching,
  current-carrying connections are exterior to the observational field
  of view, (2) the solution algorithms do not (yet) incorporate the
  measurement uncertainties in the vector magnetogram data, and/or (3)
  a better way is needed to account for the Lorentz forces within the
  layer between the photosphere and coronal base. In light of these
  issues, we conclude that it remains difficult to derive useful and
  significant estimates of physical quantities from NLFFF models.

---------------------------------------------------------
Title: A Critical Assessment of Nonlinear Force-Free Field Modeling
    of the Solar Corona for Active Region 10953
Authors: De Rosa, Marc L.; Schrijver, Carolus J.; Barnes, Graham;
   Leka, K. D.; Lites, Bruce W.; Aschwanden, Markus J.; Amari, Tahar;
   Canou, Aurélien; McTiernan, James M.; Régnier, Stéphane; Thalmann,
   Julia K.; Valori, Gherardo; Wheatland, Michael S.; Wiegelmann, Thomas;
   Cheung, Mark C. M.; Conlon, Paul A.; Fuhrmann, Marcel; Inhester,
   Bernd; Tadesse, Tilaye
2009ApJ...696.1780D    Altcode: 2009arXiv0902.1007D
  Nonlinear force-free field (NLFFF) models are thought to be viable
  tools for investigating the structure, dynamics, and evolution of
  the coronae of solar active regions. In a series of NLFFF modeling
  studies, we have found that NLFFF models are successful in application
  to analytic test cases, and relatively successful when applied
  to numerically constructed Sun-like test cases, but they are less
  successful in application to real solar data. Different NLFFF models
  have been found to have markedly different field line configurations
  and to provide widely varying estimates of the magnetic free energy in
  the coronal volume, when applied to solar data. NLFFF models require
  consistent, force-free vector magnetic boundary data. However,
  vector magnetogram observations sampling the photosphere, which is
  dynamic and contains significant Lorentz and buoyancy forces, do not
  satisfy this requirement, thus creating several major problems for
  force-free coronal modeling efforts. In this paper, we discuss NLFFF
  modeling of NOAA Active Region 10953 using Hinode/SOT-SP, Hinode/XRT,
  STEREO/SECCHI-EUVI, and SOHO/MDI observations, and in the process
  illustrate three such issues we judge to be critical to the success of
  NLFFF modeling: (1) vector magnetic field data covering larger areas
  are needed so that more electric currents associated with the full
  active regions of interest are measured, (2) the modeling algorithms
  need a way to accommodate the various uncertainties in the boundary
  data, and (3) a more realistic physical model is needed to approximate
  the photosphere-to-corona interface in order to better transform the
  forced photospheric magnetograms into adequate approximations of nearly
  force-free fields at the base of the corona. We make recommendations
  for future modeling efforts to overcome these as yet unsolved problems.

---------------------------------------------------------
Title: Nonlinear Force-Free Magnetic Field Modeling of the Solar
Corona: A Critical Assessment
Authors: De Rosa, M. L.; Schrijver, C. J.; Barnes, G.; Leka, K. D.;
   Lites, B. W.; Aschwanden, M. J.; McTiernan, J. M.; Régnier, S.;
   Thalmann, J.; Valori, G.; Wheatland, M. S.; Wiegelmann, T.; Cheung,
   M.; Conlon, P. A.; Fuhrmann, M.; Inhester, B.; Tadesse, T.
2008AGUFMSH41A1604D    Altcode:
  Nonlinear force-free field (NLFFF) modeling promises to provide accurate
  representations of the structure of the magnetic field above solar
  active regions, from which estimates of physical quantities of interest
  (e.g., free energy and helicity) can be made. However, the suite of
  NLFFF algorithms have so far failed to arrive at consistent solutions
  when applied to cases using the highest-available-resolution vector
  magnetogram data from Hinode/SOT-SP (in the region of the modeling
  area of interest) and line-of-sight magnetograms from SOHO/MDI (where
  vector data were not been available). It is our view that the lack of
  robust results indicates an endemic problem with the NLFFF modeling
  process, and that this process will likely continue to fail until (1)
  more of the far-reaching, current-carrying connections are within the
  observational field of view, (2) the solution algorithms incorporate
  the measurement uncertainties in the vector magnetogram data, and/or
  (3) a better way is found to account for the Lorentz forces within
  the layer between the photosphere and coronal base. In light of these
  issues, we conclude that it remains difficult to derive useful and
  significant estimates of physical quantities from NLFFF models.

---------------------------------------------------------
Title: Coronal Magnetic Field Extrapolation from Photospheric
    Measurements Applied to an Active Region
Authors: Fuhrmann, M.; Kliem, B.; Valori, G.; Seehafer, N.
2008ESPM...12.3.37F    Altcode:
  We outline an MHD relaxation method that permits to extrapolate
  photospheric vector magnetograms into coronal nonlinear force-free
  fields. The method is applied to a magnetogram taken before an eruptive
  event in NOAA AR 7792 on 25 October 1994. The event produced a coronal
  mass ejection (CME) and eruptive flare with a prominent sigmoidal
  soft X-ray source. Multiwavelength observations as well as theoretical
  modeling indicate the importance of twisted magnetic configurations in
  solar active regions(ARs) in the initiation of such events. Manoharan
  et al. (1996) proposed a model for this event that included the merging
  of two slightly twisted flux bundles near the polarity inversion line
  into a flux rope of larger total twist and an overlying flux system much
  closer to a potential-field state. For the extrapolation we use a vector
  magnetogram taken at the Mees Solar Observatory 16 hours before the
  actual event. The magnetic field extrapolation is able to recover main
  parts of the structures suggested in the model by Manoharan et al. We
  find the overlying nearly potential flux and part of the sigmoidal
  field, i.e., one of the suggested weakly twisted flux bundles, in the
  location observed. This supports the notion that sigmoids are coronal
  manifestations of twisted magnetic flux tubes which start expanding in
  eruptive events and may exist even before the onset of such events. We
  tentatively attribute the incomplete reconstruction of the sigmoidal
  field structure to the strong evolution of the photospheric field at
  the suggested location of flux tube merging between the time of the
  magnetogram and the eruption, as indicated by a magnetogram on the
  following day.

---------------------------------------------------------
Title: Magnetofrictional Extrapolations of Current-Carrying Flux Ropes
Authors: Valori, G.; Kliem, B.; Toeroek, T.
2008ESPM...12.2.90V    Altcode:
  The quiescent solar corona is regularly modified by very fast ejections
  of coronal material and magnetic field (CME) that occur preferably
  above active regions. Most CME models require the formation of twisted
  magnetic field structures (flux ropes) before or during such events. <P
  />Unfortunately, the coronal magnetic field is not directly measurable
  at present, and therefore it is difficult to verify the validity
  of different CME models. <P />In order to remove this obstacle, the
  extrapolation of photospheric magnetic field measurements can be used
  to reconstruct the missing coronal information. As an application of
  our magneto-frictional code, we present an extrapolation of a measured
  magnetogram where a flux rope is found. <P />In such applications it
  is necessary to estimate how well our extrapolation code can reproduce
  all aspects of highly nonlinear structures such as flux ropes. This is
  of course possible only using test fields. <P />The Titov and Demoulin
  force-free equilibrium (Titov and Demoulin, Astr. and Astrophys. 351,
  707, (1999), hereafter TD) models a semi-circular, 3D current-carrying
  flux rope by means of a current ring embedded in a potential field. The
  parameters of the TD model can be adjusted to create both stable and
  kink- and torus-unstable configurations. <P />Its solar relevance
  was confirmed by the quantitative reproduction of some specific CME
  features (see e.g., Toeroek and Kliem, Astroph. J. Lett. 630 L97
  (2005)). <P />Therefore, the TD solution is by far the most realistic
  analytical equilibrium available to date for the modeling of solar
  active regions. <P />Employing the TD equilibrium as a test-field,
  we show that the magnetofrictional extrapolation code can reproduce
  the energy and the twist of the magnetic field within a percent
  accuracy. <P />This information is essential for the reconstruction
  of coronal fields involved in eruptions because the twist is,
  together with the height profile of the overlying potential field,
  the most important stability parameter -- at least as long as the
  TD equilibrium is a good model of the considered active region. <P
  />Perfectly reproduced are also X-type magnetic topology features,
  sometimes referred to as Hyperbolic Flux Tubes, which are regarded to be
  essential to the physics of CMEs and flares because they are preferred
  locations for the formation of current sheets. <P />On the other hand,
  we also show how the scale-height of the potential field that is used
  as initial condition in the extrapolation influences the quality of the
  reconstructed field: different initial conditions reproduce correctly
  the twist and the topology, but less accurately the height and the
  shape of the flux rope. <P />Consequently, care must be taken when
  comparing the shapes of soft X-ray and EUV loops, especially those in
  the nearly potential field overlying filaments, with the field lines
  obtained from the extrapolation of the corresponding magnetogram.

---------------------------------------------------------
Title: Non-Linear Force-Free Field Modeling of a Solar Active Region
    Around the Time of a Major Flare and Coronal Mass Ejection
Authors: De Rosa, M. L.; Schrijver, C. J.; Metcalf, T. R.; Barnes,
   G.; Lites, B.; Tarbell, T.; McTiernan, J.; Valori, G.; Wiegelmann,
   T.; Wheatland, M.; Amari, T.; Aulanier, G.; Démoulin, P.; Fuhrmann,
   M.; Kusano, K.; Régnier, S.; Thalmann, J.
2008AGUSMSP31A..06D    Altcode:
  Solar flares and coronal mass ejections are associated with rapid
  changes in coronal magnetic field connectivity and are powered by
  the partial dissipation of electrical currents that run through
  the solar corona. A critical unanswered question is whether the
  currents involved are induced by the advection along the photosphere
  of pre-existing atmospheric magnetic flux, or whether these currents
  are associated with newly emergent flux. We address this problem by
  applying nonlinear force-free field (NLFFF) modeling to the highest
  resolution and quality vector-magnetographic data observed by the
  recently launched Hinode satellite on NOAA Active Region 10930 around
  the time of a powerful X3.4 flare in December 2006. We compute 14
  NLFFF models using 4 different codes having a variety of boundary
  conditions. We find that the model fields differ markedly in geometry,
  energy content, and force-freeness. We do find agreement of the best-fit
  model field with the observed coronal configuration, and argue (1)
  that strong electrical currents emerge together with magnetic flux
  preceding the flare, (2) that these currents are carried in an ensemble
  of thin strands, (3) that the global pattern of these currents and
  of field lines are compatible with a large-scale twisted flux rope
  topology, and (4) that the ~1032~erg change in energy associated with
  the coronal electrical currents suffices to power the flare and its
  associated coronal mass ejection. We discuss the relative merits of
  these models in a general critique of our present abilities to model
  the coronal magnetic field based on surface vector field measurements.

---------------------------------------------------------
Title: Nonlinear Force-free Field Modeling of a Solar Active Region
    around the Time of a Major Flare and Coronal Mass Ejection
Authors: Schrijver, C. J.; DeRosa, M. L.; Metcalf, T.; Barnes, G.;
   Lites, B.; Tarbell, T.; McTiernan, J.; Valori, G.; Wiegelmann, T.;
   Wheatland, M. S.; Amari, T.; Aulanier, G.; Démoulin, P.; Fuhrmann,
   M.; Kusano, K.; Régnier, S.; Thalmann, J. K.
2008ApJ...675.1637S    Altcode: 2007arXiv0712.0023S
  Solar flares and coronal mass ejections are associated with rapid
  changes in field connectivity and are powered by the partial dissipation
  of electrical currents in the solar atmosphere. A critical unanswered
  question is whether the currents involved are induced by the motion of
  preexisting atmospheric magnetic flux subject to surface plasma flows or
  whether these currents are associated with the emergence of flux from
  within the solar convective zone. We address this problem by applying
  state-of-the-art nonlinear force-free field (NLFFF) modeling to the
  highest resolution and quality vector-magnetographic data observed
  by the recently launched Hinode satellite on NOAA AR 10930 around
  the time of a powerful X3.4 flare. We compute 14 NLFFF models with
  four different codes and a variety of boundary conditions. We find
  that the model fields differ markedly in geometry, energy content,
  and force-freeness. We discuss the relative merits of these models in
  a general critique of present abilities to model the coronal magnetic
  field based on surface vector field measurements. For our application
  in particular, we find a fair agreement of the best-fit model field
  with the observed coronal configuration, and argue (1) that strong
  electrical currents emerge together with magnetic flux preceding the
  flare, (2) that these currents are carried in an ensemble of thin
  strands, (3) that the global pattern of these currents and of field
  lines are compatible with a large-scale twisted flux rope topology,
  and (4) that the ~10<SUP>32</SUP> erg change in energy associated with
  the coronal electrical currents suffices to power the flare and its
  associated coronal mass ejection.

---------------------------------------------------------
Title: Nonlinear Force-Free Modeling of Coronal Magnetic
    Fields. II. Modeling a Filament Arcade and Simulated Chromospheric
    and Photospheric Vector Fields
Authors: Metcalf, Thomas R.; De Rosa, Marc L.; Schrijver, Carolus J.;
   Barnes, Graham; van Ballegooijen, Adriaan A.; Wiegelmann, Thomas;
   Wheatland, Michael S.; Valori, Gherardo; McTtiernan, James M.
2008SoPh..247..269M    Altcode: 2008SoPh..tmp...17M
  We compare a variety of nonlinear force-free field (NLFFF) extrapolation
  algorithms, including optimization, magneto-frictional, and Grad -
  Rubin-like codes, applied to a solar-like reference model. The model
  used to test the algorithms includes realistic photospheric Lorentz
  forces and a complex field including a weakly twisted, right helical
  flux bundle. The codes were applied to both forced "photospheric" and
  more force-free "chromospheric" vector magnetic field boundary data
  derived from the model. When applied to the chromospheric boundary data,
  the codes are able to recover the presence of the flux bundle and the
  field's free energy, though some details of the field connectivity are
  lost. When the codes are applied to the forced photospheric boundary
  data, the reference model field is not well recovered, indicating
  that the combination of Lorentz forces and small spatial scale
  structure at the photosphere severely impact the extrapolation of the
  field. Preprocessing of the forced photospheric boundary does improve
  the extrapolations considerably for the layers above the chromosphere,
  but the extrapolations are sensitive to the details of the numerical
  codes and neither the field connectivity nor the free magnetic energy in
  the full volume are well recovered. The magnetic virial theorem gives
  a rapid measure of the total magnetic energy without extrapolation
  though, like the NLFFF codes, it is sensitive to the Lorentz forces in
  the coronal volume. Both the magnetic virial theorem and the Wiegelmann
  extrapolation, when applied to the preprocessed photospheric boundary,
  give a magnetic energy which is nearly equivalent to the value derived
  from the chromospheric boundary, but both underestimate the free
  energy above the photosphere by at least a factor of two. We discuss
  the interpretation of the preprocessed field in this context. When
  applying the NLFFF codes to solar data, the problems associated with
  Lorentz forces present in the low solar atmosphere must be recognized:
  the various codes will not necessarily converge to the correct, or
  even the same, solution.

---------------------------------------------------------
Title: Force-free magnetic fields in the solar atmosphere
Authors: Seehafer, N.; Fuhrmann, M.; Valori, G.; Kliem, B.
2007AN....328.1166S    Altcode:
  Reliable measurements of the solar magnetic field are restricted to the
  level of the photosphere. For about half a century attempts have been
  made to calculate the field in the layers above the photosphere, i.e. in
  the chromosphere and in the corona, from the measured photospheric
  field. The procedure is known as magnetic field extrapolation. In
  the superphotospheric parts of active regions the magnetic field is
  approximately force-free, i.e. electric currents are aligned with the
  magnetic field. The practical application to solar active regions has
  been largely confined to constant-α or linear force-free fields, with
  a spatially constant ratio, α, between the electric current and the
  magnetic field. We review results obtained from extrapolations with
  constant-α force-free fields, in particular on magnetic topologies
  favourable for flares and on magnetic and current helicities. Presently,
  different methods are being developed to calculate non-constant-α or
  nonlinear force-free fields from photospheric vector magnetograms. We
  also briefly discuss these methods and present a comparison of a linear
  and a nonlinear force-free magnetic field extrapolation applied to
  the same photospheric boundary data.

---------------------------------------------------------
Title: Preprocessing of solar vector magnetograms for force-free
    magnetic field extrapolation
Authors: Fuhrmann, M.; Seehafer, N.; Valori, G.
2007A&A...476..349F    Altcode:
  Context: Reliable measurements of the solar magnetic field are
  restricted to the phoptosphere. As an alternative to measurements,
  the field in the higher layers of the atmosphere is calculated from
  the measured photospheric field, mostly under the assumption that
  it is force-free. However, the magnetic field in the photosphere
  is not force-free. Moreover, most methods for the extrapolation of
  the photospheric magnetic field into the higher layers prescribe the
  magnetic vector on the whole boundary of the considered volume, which
  overdetermines the force-free field. Finally, the extrapolation methods
  are very sensitive to small-scale noise in the magnetograph data,
  which, however, if sufficienly resolved numerically, should affect the
  solution only in a thin boundary layer close to the photosphere. <BR
  />Aims: A new method for the preprocessing of solar photospheric vector
  magnetograms has been developed that, by improving their compatibility
  with the condition of force-freeness and removing small-scale noise,
  makes them more suitable for extrapolations into three-dimensional
  nonlinear force-free magnetic fields in the chromosphere and corona. <BR
  />Methods: A functional of the photospheric field values is minimized
  whereby the total magnetic force and the total magnetic torque on the
  considered volume above the photosphere, as well as a quantity measuring
  the degree of small-scale noise in the photospheric boundary data,
  are simultaneously made small. For the minimization, the method of
  simulated annealing is used and the smoothing of noisy magnetograph
  data is attained by windowed median averaging. <BR />Results: The
  method was applied to a magnetogram derived from a known nonlinear
  force-free test field to which an artificial noise had been added. The
  algorithm recovered all main structures of the magnetogram and removed
  small-scale noise. The main test was to extrapolate from the noisy
  photospheric vector magnetogram before and after the preprocessing. The
  preprocessing was found to significantly improve the agreement of the
  extrapolated with the exact field.

---------------------------------------------------------
Title: Magnetofrictional Extrapolations of Low and Lou's Force-Free
    Equilibria
Authors: Valori, G.; Kliem, B.; Fuhrmann, M.
2007SoPh..245..263V    Altcode:
  We present a careful investigation of the magnetofrictional relaxation
  and extrapolation technique applied to the reconstruction of two test
  fields. These fields are taken from the family of nonlinear force-free
  magnetic equilibria constructed by Low and Lou (Astrophys. J.352,
  343, 1990), which have emerged as standard tests for extrapolation
  techniques in recent years. For the practically relevant case that
  only the field values in the bottom plane of the considered volume
  (vector magnetogram) are used as input information (i.e., not including
  the knowledge about the test field at the side and top boundaries),
  the test field is reconstructed to a higher accuracy than obtained
  previously. Detailed diagnostics of the reconstruction accuracy
  show that the implementation of fourth-order spatial discretization
  was essential to reach this accuracy for the given test fields
  and to achieve near machine precision in satisfying the solenoidal
  condition. Different variants of boundary conditions are tested,
  which all yield comparable accuracy. In its present implementation,
  the technique yields a scaling of computing time with total number of
  grid points only slightly below N<SUP>5/3</SUP>, which is too steep
  for applications to large (≥1024<SUP>2</SUP>) magnetograms, except
  on supercomputers. Directions for improvement are outlined.

---------------------------------------------------------
Title: Non-linear Force-free Modeling Of Coronal Magnetic Fields
Authors: Metcalf, Thomas R.; De Rosa, M. L.; Schrijver, C. J.; Barnes,
   G.; van Ballegooijen, A.; Wiegelmann, T.; Wheatland, M. S.; Valori,
   G.; McTiernan, J. M.
2007AAS...210.9102M    Altcode: 2007BAAS...39..204M
  We compare a variety of nonlinear force-free field (NLFFF)
  extrapolation algorithms, including optimization, magneto-frictional,
  and Grad-Rubin-like codes, applied to a solar-like reference
  model. The model used to test the algorithms includes realistic
  photospheric Lorentz forces and a complex field including a weakly
  twisted, right helical flux bundle. The codes were applied to both
  forced "photospheric” and more force-free "chromospheric” vector
  magnetic field boundary data derived from the model. When applied to
  the <P />chromospheric boundary data, the codes are able to recover
  the presence of the flux bundle and the field's free energy, though
  some details of the field connectivity are lost. When the codes are
  applied to the forced photospheric boundary data, the reference
  model field is not well recovered, indicating that the Lorentz
  forces on the photosphere severely impact the extrapolation of the
  field. Preprocessing of the photospheric boundary does improve the
  extrapolations considerably, although the results depend sensitively
  on the details of the numerical codes. When applying the NLFFF codes
  to solar data, the problems associated with Lorentz forces present in
  the low solar atmosphere must be recognized: the various codes will
  not necessarily converge to the correct, or even the same, solution.

---------------------------------------------------------
Title: Testing non-linear force-free coronal magnetic field
    extrapolations with the Titov-Démoulin equilibrium
Authors: Wiegelmann, T.; Inhester, B.; Kliem, B.; Valori, G.;
   Neukirch, T.
2006A&A...453..737W    Altcode: 2006astro.ph.12650W
  Context.As the coronal magnetic field can usually not be measured
  directly, it has to be extrapolated from photospheric measurements
  into the corona. <BR />Aims.We test the quality of a non-linear
  force-free coronal magnetic field extrapolation code with the help of
  a known analytical solution.<BR />Methods. The non-linear force-free
  equations are numerically solved with the help of an optimization
  principle. The method minimizes an integral over the force-free
  and solenoidal condition. As boundary condition we use either the
  magnetic field components on all six sides of the computational box
  in Case I or only on the bottom boundary in Case II. We check the
  quality of the reconstruction by computing how well force-freeness
  and divergence-freeness are fulfilled and by comparing the numerical
  solution with the analytical solution. The comparison is done with
  magnetic field line plots and several quantitative measures, like the
  vector correlation, Cauchy Schwarz, normalized vector error, mean vector
  error and magnetic energy. <BR />Results.For Case I the reconstructed
  magnetic field shows good agreement with the original magnetic field
  topology, whereas in Case II there are considerable deviations from
  the exact solution. This is corroborated by the quantitative measures,
  which are significantly better for Case I.<BR />Conclusions. Despite
  the strong nonlinearity of the considered force-free equilibrium, the
  optimization method of extrapolation is able to reconstruct it; however,
  the quality of reconstruction depends significantly on the consistency
  of the input data, which is given only if the known solution is provided
  also at the lateral and top boundaries, and on the presence or absence
  of flux concentrations near the boundaries of the magnetogram.

---------------------------------------------------------
Title: Nonlinear Force-Free Modeling of Coronal Magnetic Fields Part
I: A Quantitative Comparison of Methods
Authors: Schrijver, Carolus J.; De Rosa, Marc L.; Metcalf, Thomas R.;
   Liu, Yang; McTiernan, Jim; Régnier, Stéphane; Valori, Gherardo;
   Wheatland, Michael S.; Wiegelmann, Thomas
2006SoPh..235..161S    Altcode:
  We compare six algorithms for the computation of nonlinear force-free
  (NLFF) magnetic fields (including optimization, magnetofrictional,
  Grad-Rubin based, and Green's function-based methods) by evaluating
  their performance in blind tests on analytical force-free-field models
  for which boundary conditions are specified either for the entire
  surface area of a cubic volume or for an extended lower boundary
  only. Figures of merit are used to compare the input vector field to
  the resulting model fields. Based on these merit functions, we argue
  that all algorithms yield NLFF fields that agree best with the input
  field in the lower central region of the volume, where the field and
  electrical currents are strongest and the effects of boundary conditions
  weakest. The NLFF vector fields in the outer domains of the volume
  depend sensitively on the details of the specified boundary conditions;
  best agreement is found if the field outside of the model volume is
  incorporated as part of the model boundary, either as potential field
  boundaries on the side and top surfaces, or as a potential field in
  a skirt around the main volume of interest. For input field (B) and
  modeled field (b), the best method included in our study yields an
  average relative vector error E<SUB>n</SUB> = « |B−b|»/« |B|» of
  only 0.02 when all sides are specified and 0.14 for the case where only
  the lower boundary is specified, while the total energy in the magnetic
  field is approximated to within 2%. The models converge towards the
  central, strong input field at speeds that differ by a factor of one
  million per iteration step. The fastest-converging, best-performing
  model for these analytical test cases is the Wheatland, Sturrock, and
  Roumeliotis (2000) optimization algorithm as implemented by Wiegelmann
  (2004).

---------------------------------------------------------
Title: Extrapolation of a nonlinear force-free field containing a
    highly twisted magnetic loop
Authors: Valori, G.; Kliem, B.; Keppens, R.
2005A&A...433..335V    Altcode:
  The stress-and-relax method for the extrapolation of nonlinear
  force-free coronal magnetic fields from photospheric vector
  magnetograms is formulated and implemented in a manner analogous to
  the evolutionary extrapolation method. The technique is applied to a
  numerically constructed force-free equilibrium that has a simple bipolar
  structure of the normal field component in the bottom (magnetogram)
  plane but contains a highly twisted loop and a shear (current) layer,
  with a smooth but strong variation of the force-free parameter α in
  the magnetogram. A standard linear force-free extrapolation of this
  magnetogram, using the so-called α_best value, is found to fail
  in reproducing the twisted loop (or flux rope) and the shear layer;
  it yields a loop pair instead and the shear is not concentrated in a
  layer. With the nonlinear extrapolation technique, the given equilibrium
  is readily reconstructed to a high degree of accuracy if the magnetogram
  is sufficiently resolved. A parametric study quantifies the requirements
  on the resolution for a successful nonlinear extrapolation. Permitting
  magnetic reconnection by a controlled use of resistivity improved the
  extrapolation at a resolution comparable to the smallest structures
  in the magnetogram.

---------------------------------------------------------
Title: Fluid and kinetic aspects of collisionless magnetic
    reconnection
Authors: Valori, Gherardo
2001PhDT........99V    Altcode:
  No abstract at ADS