Abstracts

Title Name Institute Abstract Title Abstract
DrAlan GabrielIAS,, Université Paris II, Orsay, France
DrAlessandra GiuntRALnull
DrAndrzej FludraSTFC Rutherford Appleton Laboratory
MrAnton RevaLebedev Physical InstituteAnomalous intensity ratio of Ly-alpha doublet hydrogen-like ion Mg XII 8.42 A in hot compact objects of the solar corona.Spectroheliograph Mg XII on the CORONAS-F satellite is an instrument which builds images of the solar corona in Ly-alpha line of hydrogen-like ion Mg XII 8.42 A. Features of spectroheliograph structure allow obtain spectrum of a doublet for compact hot objects. We investigated 169 flare-like objects, which were observed from between 20 February 2002 and 28 February 2002. Lifetime of these objects is around 2 minutes ? 3 hours, size less than 5 Mm, average temperature ? 10 MK, their intensity is below GOES A class. Intensity ratio of doublet components in these flare-like events is changing during their lifetime in the range 0,3 ? 0,7. Theoretical value is 0.5. Histogram of the ratio is symmetrical ? low values are met as often as high values. Proposed theoretical mechanism (proton excitation, satellites lines, resonance scattering) can?t explain experimental data.
DrArkadiusz BerlickiAstronomical Institute, Academy of Sciences, Czech RepublicMulti-wavelength spectroscopy of a white-light flareA. Berlicki, P. Heinzel, J. Kasparova, M. Sobotka, M. Karlicky, A. Garcia Multi-wavelength observations of o white-light flare (WLF) have been performed on August 9, 2011 close to the solar limb. We present an overview of the observational data, basic characteristics of the flare evolution (the H-alpha movie), and possible mechanisms of the WLF emission. The flare optical emission was observed around the H-alpha line with the Coimbra spectroheliograph. Luckily, the slit of the Coimbra spectroheliograph crossed the flare ribbons around the moment of the flare maximum. We clearly observe the continuum emission at +/- 15 A from the line centre, which is certainly not due to extended wings of the H-alpha line. We performed the absolute calibration of the optical spectra and study possible mechanisms of such continuous emission. We also present other observations of this event (RHESSI, SDO/AIA, SDO/EVE, radio-microwave) and use them to find the spatial and time correlations between the white-light emission and non-thermal electron bombardment of the chromosphere.
DrBart De PontieuLockheed Martin Solar & Astrophysics LaboratoryObservations and Modeling of the Chromosphere-Corona ConnectionI will review recent observations and numerical modeling of the connection between the chromosphere and corona, focusing on two phenomena, spicules and Alfven waves, that have recently been implicated in the mass and energy transfer between the low atmosphere and corona. I will discuss the potential role of spicules in explaining spectroscopic observations of Doppler shifts, line broadening and line asymmetries in the transition region and corona. I will also review the intimate coupling between both phenomena, and describe how to reconcile spectroscopic and imaging observations of Alfven waves in the corona.
MrBrendan O DwyerUniversity of CambridgeObservations of Active Region EvolutionB. O Dwyer, D. Tripathi, H. E. Mason We examine the evolution of active regions NOAA 11057 and NOAA 11193 over the course of a solar rotation, using simultaneous observations from Hinode EIS and SDO AIA. Emission measure analyses are carried out in the core of both active regions in order to investigate variations in temperature structure as the active regions evolve.
DrBrian C. Fawcett.Retired from Rutherford Appleton Laboratory.History and highlights of the identification of Solar Flare Spectra of Fe XVIII-Fe XXVI and other ions.History and highlights of the identification of Solar Flare Spectra of Fe XVIII-Fe XXVI and other ions. B. C. Fawcett: Retired from Rutherford Appleton Laboratory. Before solar flare diagnosis could start it was necessary to identify solar flare lines. No crystal soft X-ray solar spectra were available until a Naval Research Laboratory rocket flight of 1963. The first flare line of Fe XVIII was retrieved with a University College London/Leicester University rocket payload in 1966. George Doschek took part in the analysis of solar flare spectra after he joined the Naval research Laboratory in 1968. He studied satellite spectra acquired from NRL's instruments on OSO IV and OSO VI and later from SKYLAB and P 78-1 in which NRL participated. To respond to the urgent need for atomic structure flare line classifications, research using laser produced plasmas and other light sources was undertaken at NRL. This program was closely related to research, firstly conducted at Culham and then at RAL. International laboratories joined in the race with both ground based and satellite projects such as: OVI-10, 7, OSO 3, 5, 7 and intercosmos. By the time the line lists became available from P 78-1 in 1980&85 and Solar Maximum Mission in 1982&87 the main flare line identifications essential for solar spectroscopy were documented. Parallel grazing incidence studies contributed new solar flare allowed and forbidden line identifications. This presentation describes the critical atomic structure analysis involved and highlights information of special interest. After this successful research the teams moved on in the late 1980,s to participate, across Pacific as well as the Atlantic, in great space projects, such as those presented at this Conference, which often rely on these line identifications.
DrBrigitte SchmiederObservatoire de Paris, LESIASpectroscopic diagnostics for prominenceSchmieder B., Heinzel P., Gunar S., Mein P., Labrosse, N., Berlicki A. The dynamics of prominence fine structures is a challenge to understand the formation of cool plasma prominence embedded in the hot corona. The observations of fine structures obtained by different spectrographs on the ground (MSDP/Meudon) and in space (Hinode/EIS, SOHO/SUMER) combined with 2D non ?LTE radiative transfer code allow us to study the bulk velocities in these structures. The Dopplershifts of bright threads measured by the MSDP spectrograph of a hedge-row prominence observed by Hinode/SOT are of the same order of magnitude larger than the velocities perpendicular to the line-of-sight . This statement suggests that the vertical structures shown in SOT movies are not real vertical magnetic structures but a pile up of dips along horizontal field lines. Thermal characteristics of the plasma in prominence and its environment are derived from the study of hydrogen Lyman lines and transition region lines using SUMER . Hinode/EIS give some insight of the bubble?? temperature below prominences. The rise of the bubble would be due more to magnetic instability than thermal effect.
ProfCarole JordanUniversity of OxfordEmission line profiles in solar and stellar ultraviolet spectraCarole Jordan The profiles of uv emission lines yield important information on line broadening and velocity fields, and have been studied, with increasing accuracy, since the early days of solar observations from space. The spectra of quiet solar regions, from the chromosphere to the corona (including density-sensitive lines), allow constraints to be placed on the non-thermal energy densities and fluxes associated with processes that might heat the quiet corona. The Space Telescope Imaging Spectrograph on the Hubble Space Telescope provides the highest quality uv spectra available, although for spatially integrated emitting regions. For both solar and stellar sources, line shifts and two-component profiles are observed, which further constrain processes present. While stellar sources give dependencies on properties such as the surface gravity, effective temperature and rotation period, solar observations above the limb provide the only means of examining the high corona where energy dissipation is most likely to occur.
DrCostis GontikakisResearch Center for Astronomy and Applied Mathematics, Academy of AthensStudy of flows and the three-dimensional shape of coronal loops observed by Hinode/EIS.Authors: C. Gontikakis, P. Syntelis, M.K. Georgoulis, C.E. Alissandrakis, and K. Tsinganos Abstract text : We study plasma flows along selected coronal loops in NOAA Active Region 10926, observed on December 3, 2006 with Hinode EUV Imaging Spectrograph (EIS). From the shape of the loops traced on intensity images and the Doppler shifts measured along their length we compute their three-dimensional (3D) shape and plasma flow velocity using a simple geometrical model. This calculation was performed for loops visible in the Fe VIII 185A, Fe X 184A, Fe XII 195A, Fe XIII 202A, and Fe XV 284A spectral lines. For the 6 loops, studied in 16 different images, we find cases with unidirectional flows and also cases of draining motions from the loops' top to their footpoints. Our results indicate that the same loop may show different flow patterns when observed in different spectral lines, suggesting dynamically complex rather than monolithic structures. We have also carried out magnetic field extrapolations using SOHO/MDI magnetograms, aiming toward a first-order identification of extrapolated magnetic field lines corresponding to the reconstructed loops. In all cases, the best-fit extrapolated lines exhibit left-handed twist, in agreement with the dominant twist of the region.
DrDavid BrooksGeorge Mason University
DrDavid LongMSSL/UCL
MrDavid SheltonUCL/MSSLThe onset of outflows in NOAA 11117 using SDOD.Shelton, L.Harra, L.Green Coronal outflows have been observed using EUV imaging on TRACE. However, it has only been since the launch of Hinode that direct spectroscopic detection of persistent outflows have been made using the EUV Imaging Spectrometer These persistent outflows have larger speeds in spectral lines that are formed at T > 1 MK, they are found at the edges of active regions and are unchanged over a long period of time. It has been suggested that these persistent outflows could be caused by chromospheric evaporation flow magnetic reconnection and that the outflows could be related to the origin of the slow solar wind. EIS observations show that these outflows are associated with ?open? coronal magnetic field lines. It has recently been shown that emerging flux into an active region can produce new and enhanced outflows. which have been shown through simulations to be caused by a mixture of compression and magnetic reconnection. In this work, we choose an example of a region that emerged into quiet Sun and not into a pre-existing active region. We present the results of a study using the Solar Dynamics Observatory (SDO) of the emergence of active region NOAA 11117 which was present on the solar disk between 21st October and 31st October 2010. By using the high spatial resolution and high temporal cadence of SDO, we are able to determine when in the formation of the active region that the onset of these persistent outflows started. The outflows were delayed by 3 and a half days from the region s first emergence. By comparing the AIA 171 Angstrom data with the HMI magnetogram data for this period, we see that the persistent outflows only start to appear after the leading polarity starts to coalesce.
DrDavid WilliamsUCL/MSSLHinode/EIS observations of ion kappa distributions in active regions of the solar corona. D.Williams, Ed Lee (KU Leuven), Giovanni Lapenta (KU Leuven).Solar spectroscopy traditionally assumes electrons and ions in coronal plasma exist in Maxwell?Boltzmann distributions, or thermal equilibrium. Many studies in recent decades, however, have investigated the possibility of kappa distributions of coronal and solar wind particles far from Maxwellian and their resulting effects on collision, excitation, and ionization rates, heat transfer, waves, and instabilities. Kappa distributions belong to a class of statistical equilibrium ensembles that are known solutions to the Boltzmann equation, in both collisional (Fokker-Planck) and collisionless (Vlasov) frameworks. They have been observed in situ in the solar wind and in planetary magnetospheres throughout the heliosphere. Using EIS data, we investigate the possibility of suprathermal distributions of coronal ions by fitting the equivalent kappa functions to their emission line profiles. We fit different kappa and Gaussian model functions to line profiles of the strong Fe XV line at 284.16 A, across two large-field rasters taken in an active region. Both single- and double-component Gaussian models are applied, as well as two kappa models, one with a free width parameter allowing for and the other with a constrained width that precludes 'microturbulence'. We then compare the goodness of fit of the computed best fits for each model. The kappa distribution is a generalization, or superset, of the Maxwellian, so they are able to fit line profiles more precisely than a Gaussian. In most of the data, the best-fit kappa model produces much lower residuals across the profile than any single Gaussian and sometimes double Gaussian. Most importantly, the distribution of estimated kappa values is found to lie mostly in the low-k range, implying ion populations far from Maxwellian. We find the shape of the Fe xv line, in the vast majority of the data analyzed, to be indicative of a highly suprathermal ion population.
DrDavina InnesMax-Planck-Institut fuer SonnensystemforschungTransition region explosive events at the base of mini-CMEs in the quiet SunExplosive events are characterized by broad non-Gaussian wings in their line profiles and are thought to be the result of magnetic reconnection in the transition region. SDO/AIA is now providing images of these events. By combining SDO/AIA images with SUMER spectra, the association of explosive events with He II brightenings, coronal jets, and sudden dimmings is investigated. We find several cases of explosive events seen in the O VI 1032 A line that coincide with jet-like brightenings at the base of EUV coronal dimmings (mini-CMEs). Here we show some examples and estimate the energy released in the events.
DrDeb BakerUCL/MSSLMagnetic Topology, Coronal Outflows and the Solar Windvan Driel-Gesztelyi, L., Culhane, J.C., Demoulin, P., Mandrini, C.H., DeRosa, M.L., Rouillard, A.P., Opitz, A., Stenborg, G., Vourlidas, A., Brooks, D.H. During 2-18 January 2008 a pair of low-latitude opposite polarity coronal holes were observed on the Sun flanked by two ARs with the heliospheric plasma sheet between them. Hinode/EUV Imaging Telescope (EIS) is used to locate AR-related outflows and measure their velocities. The Advanced Composition Explorer (ACE) in-situ observations are employed to assess the resulting impacts on the interplanetary solar wind (SW). Magnetic field extrapolations of the two ARs confirm that AR plasma outflows observed with EIS are co-spatial with quasi-separatrix layer locations, including the separatrix of a null point. Global potential field source-surface modeling indicates that field lines in the vicinity of the null point extend up to the source-surface, enabling a part of the EIS plasma upflows access to the SW. Similar upflow magnitude is also observed within closed field regions. Though part of the plasma upflows observed with EIS remain confined along closed coronal loops, a subset of them are indeed able to make their imprint in the slow SW, making ARs bordering coronal holes a slow SW contributor.
MrEhsan PedramMSSLCME-RELATED CHANGES IN LINE-OF-SIGHT MAGNETIC FIELD STRENGTH IN DIMMING REGIONS OBSERVED BY HINODE ON 14 DECEMBER 2006Following many coronal mass ejections (CMEs), dark areas referred to as coronal dimming regions have been observed to form within and around the erupting active region. We probe the nature of coronal dimmings in relation to the expanding CME through the analysis of the associated photospheric magnetic field in the flare and CME event of 14 December 2006, using data from Hinode?s SOT. We have systematically analysed the variation of the line-of-sight magnetic field strength in a large region surrounding AR 10930 using Hinode SOT Stokes V data. Our analysis, for the first time, shows that at the site of the dimmings there is a decrease in the magnetic field strength at the onset of the dimming in the dominant polarity of the plage regions surrounding the Active Region (AR), persisting during the dimming and recovering at the onset of the intensity recovery reported in Attrill et al. (2010). Using simple geometric arguments we show that the decrease in the dominant polarity flux is consistent with an 35 degrees change in the inclination angle of the photospheric magnetic fields in the plage regions, from horizontal to vertical. We further observe a close correlation between the site of plasma outflow with velocities of 30 km/s and one of the plage regions showing change in magnetic field strength. Our findings indicate a reconguration and opening of the magnetic field lines resulting in a change in their inclination angle in the dominant polarity of the plage regions surrounding the erupting active region. This then leads to a decrease in the plasma density observed as coronal dimming.
DrElena DzifcakovaAstronomical Institute of the Academy of Sciences of the Czech RepublicKappa-distributions: line intensities and diagnostics for Fe XI and Fe XVIIE. Dzifcakova, G. Del Zanna, H. Mason We searched for the EUV lines of Fe XI and Fe XVII in the spectral range corresponding to the EIS detectors, which allow us to diagnose the kappa-distributions. The presence of the kappa-distribution in solar corona can be connected e.g. with heating mechanisms by the magnetic reconnection. The synthetic spectra for different values of kappa, electron density, and temperature were calculated for new sets of atomic data. The type of electron distribution together with temperature and electron density affects intensity of each line. Usually, the electron density must be diagnosed first and then, for known density, selected line ratios give a possibility to diagnose kappa and temperature simultaneously. This is the case of Fe XI lines. On the other hand, the ratios of Fe XVII lines in the EIS spectral ranges are not affected by electron density. Therefore Fe XVII lines give the best opportunity for non-Maxwellian diagnostics. The line ratios with the best sensitivity to the shape of the distribution function have been selected and diagnostics of the parameter kappa has been proposed. The possibility to diagnose the kappa-distributions from EIS observations is discussed.
MsElizabeth Doscheknone
DrGeorge DoschekNaval Research Laboratory"To Be Or Not To Be" ? Be with Plan B of Solar-C!George A. Doschek, Space Science Division, Naval Research Laboratory and The Solar-C Teams. What's the future for "Spectroscopy of the Dynamic Sun"? What can we do to try to finally understand the elusive mystery of the solar atmosphere ? how is it formed, what is its detailed structure, how does it evolve, what are the fundamental physical processes involved in the interaction of the Sun's magnetic fields with hot plasma, how is energy transported, stored, and dissipated in the Sun?s atmosphere, how will we understand energy release in flares and coronal mass ejections, and coronal heating in general? I believe that imaging spectroscopy with high time resolution is the key technique for finding answers to these questions. The Japanese Hinode mission with US and UK participation has laid the groundwork for future missions. In the near future the Interface Region Imaging Spectrograph (IRIS) NASA Small Explorer Mission will start the ball rolling in obtaining high time resolution imaging spectroscopy of the chromosphere and also give us a peek into the transition region and corona. The Japanese Solar-C mission is designed to obtain imaging spectroscopy at high spatial and spectral resolution throughout the entire atmosphere, from the photosphere to multimillion degree solar flare plasmas. For the first time, a mission is being developed to study the solar atmosphere as a coupled system from the photosphere into the corona with matched instrumentation. It will require international participation to realize this fantastic state-of-the-art mission. Only with a coupled systems approach can we finally understand the fundamental physics of the solar atmosphere, and presumably the atmospheres of many other stars as well. In this talk, I will discuss the on-going planning and the essential elements of the Solar-C mission as they are currently conceived.
DrGiannina PolettoINAF - Arcetri Astrophysical Observatory - Firenze (Italy)
DrGiulio Del ZannaUniversity of CambridgeXUV spectroscopy of the solar corona and the relevant atomic dataI will briefly mention some of the important measurements of the coronal plasma characteristics that have been possible in recent years thanks to high-resolution spectroscopy from instruments such as SOHO/SUMER and Hinode/EIS. I will then provide an update on recent results I have obtained on atomic data calculations and benchmarking of the coronal iron ions, with emphasis on the EUV and Soft X-rays. The new atomic data are important for EIS and for the SDO instruments.
DrHarry WarrenNRLSpectroscopic Observations of Solar FlaresPeter Young (GMU) During the past several years new spectroscopic observations of solar flares have become available from EIS/Hinode and EVE/SDO. EVE observes every ionization stage of Fe from Fe IX to Fe XXIV and allows for the thermal structure of solar flares to be examined in detail. These measurements show that the temperature distribution is broad, even during the rise phase of the flare. This suggests heating over many different independent threads. In contrast with EVE, EIS measurements are spatially resolved. Our initial survey of EIS observations suggests that these observations show much larger velocity signatures than spatially averaged measurements, but are still unresolved. We will present comparisons with multi-thread hydrodynamic models.
DrHelen E. MasonUniversity of CambridgeCoronal Iron IonsH.E.Mason, G.Del Zanna, B.O Dwyer, P.J.Storey, N.R.Badnell Coronal iron ions give rise to spectral lines in the visible, infra-red, ultra-violet and X-rays. They have been studied for decades, from eclipse observations to space missions (Skylab, SMM, SoHO, Hinode). The first comprehensive calculations were carried out in the 1970 s using the atomic physics codes developed at UCL. Diagnostic techniques have been developed and tested against observations for a whole range of ions. The calculations and line identifications are still being refined, with recent work as part of the UK APAP project. This talk will look back on a lifetime s work to see what progress has been made.
DrHirohisa HaraNational Astronomical Observatory of JapanSpectroscopy of the site of magnetic reconnectionWe report fundamental structures near the site of magnetic reconnection in a type of solar flares that were observed by the Hinode EUV Imaging Spectrometer. They consist of a bright source at the top of flare loops, a fast outflow above the bright source, and an inflow structure. We have estimated the reconnection rate to be 0.01-0.1 from the Doppler velocity measurement by emission-line spectroscopy. The presence of slow-mode and fast-mode MHD shocks is discussed with supporting evidence based on the observed quantities.
MrHugh HudsonUC Berkeley and GlasgowEVE Spectroscopy of Solar FlaresHugh S. Hudson The EVE instrument on SDO has brought systematic EUV spectrometry to solar flare physics, albeit without imaging, at a spectral resolution of about 0.1 nm. I describe some initial results on Doppler shifts, continua, and charge-exchange signatures of high-energy particles, and discuss their implications for our understanding of flares.
ProfJ. Leonard CulhaneMSSL and ISSI
DrJaroslav DudíkFaculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, SlovakiaDiagnostics of the non-Maxwellian kappa-distributions from Hinode/EIS observationsDudik, J. (1,2), Mackovjak, S. (1,2), Dzifcakova, E. (2) (1) - Dept. of Astronomy, Physics of the Earth and Meteorology, Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia (2) - Astronomical Institute of the Academy of Sciences of the Czech Republic, Ondrejov, Czech Republic We investigate line ratios suitable for diagnostics of temperature, density, and the type of the electron distribution in the coronal and transition region spectra observed by Hinode/EIS. Density diagnostics using lines of elements other than Fe are sought. Such line ratios should not be dependent on kappa. The quality of such density diagnostics is assessed and it is found that all of the investigated density-sensitive ratios suffer from largely unknown blends. Therefore, we diagnose the density using Fe line ratios. Subsequently, we search for methods suitable for simultaneous diagnostics of kappa and temperature. We show that such diagnostics is indeed possible, but suffers from large errors due to photon noise. However, the observed O IV and O V line ratios provide indications of strong departures from the Maxwellian distribution. We discuss the implications of non-Maxwellian distributions for the coronal heating.
DrJaroslav DudíkFaculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, SlovakiaThe optically thin continuum for the non-Maxwellian distributions (Poster)Dudik, J., Kasparova, J., Dzifcakova, E., Karlicky, M., Mackovjak, S. We calculate the optically thin EUV, X-ray and radio continua arising due to free-free and free-bound transitions in the coronal and flare plasmas characterized by non-Maxwellian kappa- and n-distributions. The continua are highly dependent on the assumed type of distribution. The free-free continuum is sensitive to the type of distribution mainly in the X-ray range, but is not sensitive to the type of the distribution for radio wavelengths. The height of the ionization edges in the free-bound continua are also affected by the type of the distribution. The ionization edges disappear for n-distributions due to the decreased number of low-energy electrons, forming a smooth continuum for n > 5. For the kappa-distributions, the ionization edges are greatly increased and in principle allow for determination of kappa using the observations of the continuum. Since the height of the ionization edges depends on the number of low-energy electrons, such diagnostics allows for sampling the low-energy end of the distribution function.
DrJay BookbinderSmithsonian Astrophysical Observatory
ProfJoan SchmelzUniversity of MemphisSpectroscopy of Coronal LoopsJ. T. Schmelz, University of Memphis Without spectroscopy, what would we know about coronal loops? Would we, could we know the temperature, density, or composition of their photon- emitting plasma? Could we know their magnetic field strength and structure? Would we even know of their existence? Spectroscopy has been the key to the discovery of the million-degree corona and the dominance of the magnetic loop population. Coronal loops may yet provide the elusive answer to the coronal heating problem, and it will be spectroscopy that provides the fundamental foundation for the discovery. In this talk, I will discuss both the historical and continuing contributions of spectroscopy to coronal loop science, from Skylab?s Spectrograph and Spectroheliograph to Hinode?s EUV Imaging Spectrometer, as well as the imagers that have been based on spectroscopic science. Although we still argue about the cross-field temperature distributions, the accuracy of density-sensitive line ratios, and the elemental abundances of coronal loop plasma, it is spectroscopy itself that allows us not only to have these arguments but also to make progress on essential coronal science.
DrKelly KorreckSmithsonian Astrophysical ObservatoryPre-Flare temperature diagnostics in the EUVK.E. Korreck - SAO, A. Sturner-Haverford College EUV observations of flaring active regions in solar corona indicated a possible temperature precursor to flaring activity. SDO?s AIA instrument with its continuous full disk coverage allows for a more systematic exploration of this effect. The resolution both temporal and spatial will aid in addressing the presence and amount of pre-heating. This poster examines active regions using the SDO/AIA EUV telescopes prior to flaring events to characterize their emission in the 7 EUV bandpasses available. The link between the pre‐flare brightening and energetic particle events will also be examined. This work could prove invaluable to the prediction of space weather events such as flares.
ProfKenneth J.H. PhillipsMullard Space Science Laboratory, University College LondonSolar Flare Element Abundances from RESIK and other spectrometersK. J. H. Phillips, J. Sylwester, B. Sylwester, G. A. Doschek, J. L. Culhane, V. D. Kuznetsov. The RESIK crystal spectrometer on board CORONAS-F operated during maximum solar activity in 2002/2003, and many thousands of spectra acquired during flares as well as non-flaring times from bright active regions. George Doschek was centrally involved in the making of the instrument, providing the excellent silicon and quartz crystals with his NRL team. A detailed characterization of the various instrument parameters has led to a calibration of the spectra with unprecedented precision and the solar continuum to be unambiguously observed for two of RESIK s four channels. All this has enabled element abundances to be obtained from the fluxes of the large variety of spectral lines in the 3-6 Angstrom range. A comprehensive programme over the past 2 years has resulted in the determination of Ar and S abundances as well as those of K and Cl. A wide range of first ionization potentials are represented, so the nature of the FIP effect can be examined in a new light: thus for the low-FIP K, the abundance in flares is nearly a factor 6 more than photospheric or meteoritic, but Ar and S flare abundances are very similar to their photospheric abundances. For non- flaring active regions K is much more abundant. There is broad agreement of our derived abundances with the recent theory of Laming. The presence of the He-like K lines in RESIK spectra has led to the identification of the same lines in the spectra of RS CVn binary stars. Our method of abundance analysis has inspired us to look again at the S line spectra from the Yohkoh BCS that were studied by Tetsuya Watanabe in the 1990s. The success of the RESIK results has resulted in a proposed new crystal spectrometer, ChemiX, to be flown on the Russian Interhelioprobe spacecraft, tentatively due for launch in 2018.
DrKHELFI Researcher Propagation of p-modes in a magnetic structure with flowThe solar sub-photospheric zone is a huge reservoir of a mechanical energy generated by the convective motion which takes place in the convective zone. The perturbations induced by this motion generate a wide spectrum of acoustic waves (P modes) which have been observed at a photospheric level. Recent space based observations suggest that these P modes can manifest them- selves as slow magneto-acoustic waves while propagating in coronal magnetic structures such as coronal loops which are anchored in the solar photosphere into sunspot regions. Consequently, in order to show theoretically the possible occurrence of this scenario, we present in this work a detailed analysis of the interaction of a P mode with a sunspot under typical photospheric conditions. For this we consider a simple slab configuration made of a non-magnetized and a magnetized (sunspot) region with presence of a flow at the interface. The conditions under which an acoustic wave is transmitted into the magnetized region as a magneto-acoustic wave are studied in details. The transmission and reflection angles and the transmittance and reflectance of the magneto-acoustic wave are calculated and examined. They reveal that the transmitted wave is a slow magnetoacoustic wave which propagates upwards guided by the magnetic field which confirms the recent observations.
DrLeon GolubHarvard-Smithsonian CfA
DrLuca TeriacaMax Planck Institute for Solar System ResearchQuiet Sun electron densities from the C III 97.7/117.6 line ratioL. Teriaca, V. Andretta In a fully ionized plasma, the measurement of the electron density provides a direct measurement of the mass density, a fundamental thermodynamic variable in all studies of the solar atmosphere. The most reliable method to measure the electron density involves the ratio of spectral lines, or groups of lines, from the same ion but with substantially different spontaneous decay coefficients Normally such ratios involve very weak forbidden lines posing serious problems to the study of even slowly evolving phenomena. One of the most remarkable exception is the ratio of the C III 97.7 nm line with the C III multiplet at 117.6 nm, being both very bright features of the solar VUV spectrum. However, the 117.6 nm multiplet is potentially blended with a autoionization lines from S I. Here we evaluate the importance of such blend in different solar regions and in solar-like stars and discuss the usability of the 97.7/117.6 ratio under quiet Sun conditions.
DrMark WeberCfA / SAOMorphology and Temperature of a Hot Prominence Cavity Observed with Hinode and SDO Mark Weber (SAO), Katherine K. Reeves (SAO), Sarah E. Gibson (HAO/NCAR), and Therese A. Kucera (NASA/GSFC) Prominence cavities appear as circularly shaped voids in coronal emission over polarity inversion lines where a prominence channel is straddling the solar limb. The presence of chromospheric material suspended at coronal altitudes is a common but not necessary feature within these cavities. These voids are observed to change shape as a prominence feature rotates around the limb. We use a morphological model projected in cross-sections to fit the cavity emission in Hinode observations, and then apply temperature diagnostics to Hinode and SDO data to investigate the thermal structure. We find significant evidence that the prominence cavity is hotter than the corona immediately outside the cavity boundary. This investigation follows upon "Thermal Properties of A Solar Coronal Cavity Observed with the X-ray Telescope on Hinode" by Reeves et al., 2012, ApJ, in press. M. Weber and K.K. Reeves are supported under contract NNM07AB07C from NASA to SAO. T. Kucera is supported by an award from the NASA SHP Program.
DrMatthew WestRoyal Observatory BelgiumCoronal Seismology Using EIT Waves: Estimation Of The Coronal Magnetic Field Strength In The Quiet SunM. J. West, A. N. Zhukov, L. Dolla, L. Rodriguez Coronal EIT waves have been observed for many years. The nature of EIT waves is still contentious, however there is strong evidence that some of them might be fast magnetosonic waves, or at least have a fast magnetosonic wave component. The wave speed is formed from two components; the Alfven speed (magnetic) and the sound speed (thermal). By making measurements of the wave speed, coronal density and temperature it is possible to calculate the quiet Sun coronal magnetic field strength through coronal seismology. In this work we investigate an EIT wave observed by the SECCHI/EUVI instruments on-board the STEREO satellites. The wave epicenter was observed at disk center in the STEREO B (Behind) satellite. At this time the STEREO satellites were separated by approximately 90 degrees, and as a consequence the STEREO A (Ahead) satellite observed the wave on the solar limb. These observations allowed us to make accurate speed measurements of the wave. The background coronal density was derived through Hinode/EIS observations of the quiet Sun and the temperature was estimated through the narrow temperature response in the EUVI bandpasses. The density, temperature and speed measurements allowed us to estimate the quiet Sun coronal magnetic field strength to be approximately 0.7 ± 0.7 G.
MrNaomasa KitagawaUniversity of TokyoThe evolution of chromospheric evaporation observed with Hinode/EISN. Kitagawa & T. Yokoyama (University of Tokyo, Japan) Department of Earth and Planetary Science, University of Tokyo, Hongo 7-3-1, Bunkyo, Tokyo, 113-0033 Japan The evolution of chromospheric evaporation observed with Hinode/EIS We analyzed the ongoing chromospheric evaporation in the impulsive phase. The dense and cool plasma in the chromosphere experiences impulsive heating by nonthermal particles produced at the flare reconnection site. The gas pressure suddenly rises, which results in so called chromospheric evaporation, fast upflow with several hundreds km/s. The chromospheric evaporation was detected as the blueshifted component in Ca XIX line profiles (Antonucci et al. 1982). Czaykowska et al. (1999) firstly reported spatially resolved evaporation in the gradual phase observed with the Coronal Diagnostic Spectrometer (CDS) onboard the Solar and Heliospheric Observatory (SOHO). Recent observations by Hinode/EIS revealed more detailed structures. The temperature dependence of the evaporation velocity was reported by Milligan & Dennis (2009). The fast upflow from the footpoints of flare loops was found during the early phase (Watanabe et al. 2010; Del Zanna et al. 2011). Chen & Ding (2010) found a temporal correlation between the blueshift and line width. In this study, the enhanced blue wings (~400km/s) were found in Fe XXIII and XXIV profiles in the growing flare loops. Other coronal lines at the evaporation site also show the velocities near the sound speed in each formation temperature. The upflow is switched into downflow at several MK. Fortunately, in the data used here the EIS spectroscopic slit cut across old and new flare loops simultaneously, which enables us to discuss the temporal evolution.
DrNaoto NishizukaISAS/JAXATime variation of Active region outflow with recurrent flows and wavesNaoto Nishizuka (ISAS/JAXA) and Hirohisa Hara (NAOJ): Raster scan observations with EIS/Hinode have revealed characteristics of steady outflow from the edge of active regions. Furthermore, recent observations of EIS with sit-and-stare mode have also revealed unsteady features of the AR outflow. Here we report the sit-and-stare observation data of NOAA 10942 on 2007 February 20 and analyzed the data above the base of the outflow and found both continuous outflows and waves, which propagate from the base of the outflow. The spectra at the base of the outflow and at higher locations show different properties. The line profiles show blue-side asymmetry at the base of the outflow where nonthermal broadening becomes large because of fast upflows generated by heating events. On the other hand, at higher locations line profiles are symmetric and the intensity disturbances vary in phase with the velocity disturbances, indicating upward propagating slow-mode waves. High cadence spectroscopic observations revealed intermittent signatures of nonthermal velocities with 2 minutes period and 2?? size. Each of them seems to correspond to the base of the propagating disturbances. The similarity of line profiles of the outflow and the jet may indicate that the flows and waves originate in unresolved explosive events in the lower atmosphere of the corona.
MsNeda DadashiMax Planck Institute for Solar System ResearchDoppler shift of hot coronal lines in a Moss Area of an Active regionN. Dadashi, L. Teriaca, D. Tripathi, S. K. Solanki We use a novel technique that allows determining the absolute Doppler shift of EUV lines by combining observations from the SUMER and EIS spectrometers. This technique, developed and successfully applied to quiet Sun data, is now used to investigate the absolute Doppler shift of lines formed at temperatures between 1 MK and 2.5 MK in a moss area within active region NOAA 11243. The moss is the area at the footpoint of the hot (3 to 5 MK) loops forming the core of the active region where emission is believed to result from the heat flux conducted down to the transition region from the hot loops. Thus, studying the variation of Doppler velocity over the moss area can give clues on the heating mechanism in the hot loops in the core of the active regions. Preliminarily results for the center of the moss area shows roughly constant blue shift (upward motions) of -5 km/s in the temperature range of 1MK to 1.6MK. For hotter lines the amount of upward motions decrease and reaches to -1 km/s for Fe XV 284. The measurements are discussed with respect to models of the heating of such hot loops.
MrOYELEKE OLAOSEBIKANTHE FEDERAL POLYTECHNIC OFFA, KWARA STATE, LADOKE AKINTOLA UNIVERSITY OF TECHNOLOGY, OGBOMOSOComparative study of the output of Amorphous Silicon Photovoltaic Solar Cells when receiving Direct and Diffused RadiationsAuthor: Oyeleke, O (1) Co-Author: Fajinmi, G.F (2) Four Amorphous Silicon Photovoltaic cells rated 12V, 20amps, 30watt DC were subjected to solar radiations study with the aim to determining their output at different positions. The four amorphous Silicon Photovoltaic were paired in two. A pair was placed on a sun tracker while the other was placed on a fixed position. An LDR cell was constructed to control the tracking system while an LED was connected ton indicate the radiation intensity at a particular time. The output power for both arrangements were recorded at 10minutes interval for a period of two months. The data obtained were compared and treated to obtain a model of mean output power at a particular temperature for the two pairs separately. It was observed that the mean output power of the setup on tracking mechanism has a higher mean output power.
DrP. F. ChenUCL/MSSL & Nanjing UniversityThe puzzling red shift behind the coronal EIT waveP. F. Chen and L. K. Harra Generally blue-shifted outflows are associated with dimmings which expand behind EIT waves, which can be understood since magnetic field lines are stretched up during the eruption, taking along with the coronal plasma. With the high-cadence sit-and-stare mode of the Hinode/EIS observations, Harra et al. (2011) found two waves in the coronal lines, with the faster one being a coronal Moreton wave, and the slower one probably being an EIT wave. Following the slower wave, Hinode/EIS did show blue shifts. However, the blue shifts soon turned to be red shift, which is a little puzzling. With MHD numerical simulations of coronal mass ejections (CMEs), we try to understand how the red shifts are formed below the CME eruption.
DrPaola TestaHarvard-Smithsonian Center for AstrophysicsCombined AIA/EIS diagnostics for high temperature plasma in active regionsWe use coronal imaging observations with SDO/AIA, and Hinode/EIS spectral data, to explore the potential of narrow band EUV imaging data for diagnosing the presence of hot (T > 5MK) coronal plasma in active regions. We analyze observations of two active regions with simultaneous AIA imaging, and EIS spectral data, including the CaXVII line which is sensitive to hot coronal plasma even outside flares. After careful co-alignment of the imaging and spectral data, we compare the morphology in a 3 color image combining the 171, 335, and 94A AIA spectral bands, with the image obtained for CaXVII emission from the analysis of EIS spectra. We find that in the selected active regions the CaXVII emission is strong only in very limited areas, showing striking similarities with the features bright in the 94A AIA channels and weak in the 171A band. We conclude that AIA imaging observations of the solar corona can be used to track hot plasma, and thus to study its spatial variability and temporal evolution at high spatial and temporal resolution.
MrPatrick Serenguliannone
DrPavel KotrcAstronomical Institute, Academy of Sciences, Ondrejov, Czech RepublicSpectroscopic study of solar filaments/prominences ? ground based observations.Kotrc P.(1), Schwartz P.(1) and Kupryakov Yu. A.(2) (1)Astronomical Institute, Ondřejov, Czech Republic, (2) GAISH, MGU, Moscow, Russia We present an overview of tools and methods we use for a multispectral study of solar filaments and their EUV channels. Particularly, we concentrate on using and description of the ground based part of the project ? the spectroscopic observations of filament and prominences. Spectra nad filtergrams of a large set of quiescent prominences/filaments observed at the Ondrejov laboratory spectrograph are used for determinantion of optical thickness and integral intensity in the H-alpha line. The main aim is to contribute to multiwavelength analysis and computations of the prominence/filament mass loading. We want to study distribution and limits of the prominence mass interval in more details.
DrPavol SchwartzAstronomical Institute, Academy of Sciences of the Czech RepublicProminence mass estimated from multi-spectral dataP. Schwartz, P. Heinzel, P. Kotrc, U. Anzer and Yu. A. Kupryakov A spectroscopic method for estimation of the total mass of a prominence from multi-spectral observations was developed. Observations in EUV by AIA instrument on board of SDO, in soft X-rays by XRT on Hinode and in H_alpha by MFS spectrograph of the Ondrejov observatory are used. The total mass of a prominence is obtained by integration over the whole prominence area, of the column mass derived from column densities which are obtained using a semi-automatic code developed according to the method of Heinzel et al. (2008). Non-symmetrical distributions of the coronal X-ray and EUV emissivities in front of and behind the prominence is taken into account as well. We use the so-called alpha factor defining a fraction of the emissivity behind the prominence. The mass determination then depends on the correct specification of this factor. Alpha factor is estimated iteratively by comparing a ratio of the optical thicknesses at 193 A and 211 A derived from observations with the theoretical value calculated according to Anzer & Heinzel (2005). The robustness of the method is tested on several prominences and derived alpha values are compared with approximate value obtained from the intensities measured on the disk and at the limb close to a prominence.
DrPeter YoungGeorge Mason UniversityAdvances in solar spectroscopy from Hinode/EISTetsuya Watanabe and George Doschek were instrumental in developing and leading the Hinode/EIS project, which has led to great advances in the application of spectroscopic techniques for studying the solar corona. EIS directly benefited from Tetsuya and George s experience in solar spectroscopy as the wavelength bands they helped select gave access to some of the best plasma diagnostics at coronal temperatures. This presentation will focus on new science that has become possible with EIS, with particular attention to density diagnostics and velocity measurements in active regions.
ProfPetr HeinzelAstronomical Institute, Academy of Sciences, Czech RepublicSDO/EVE spectra of solar flares: Non-LTE models of EUV continua P. Heinzel, E.H. Avrett, E. Dzifcakova, A. Berlicki For selected flare events we present the SDO/EVE spectra of hydrogen and helium EUV resonance continua and compare them with the results of the non-LTE transfer computations based on various flare models. We discuss the formation of these continua and their diagnostic potential for determination of the temperature structure of the flaring atmosphere. Non-thermal processes are also considered. This work represents the basis for future analysis of the EVE flare spectra and has also a direct relevance to stellar flare spectroscopy.
DrRandall SmithSmithsonian Astrophysical ObservatorySolar and Stellar Spectroscopy with X-ray MicrocalorimetersJay Bookbinder (SAO), Simon Bandler and the NASA/GSFC calorimeter team We present the science case for a broadband X-ray imager with high-resolution spectroscopy for both stellar and solar observations. In the solar case, high- resolution X-ray spectral images of both active regions and solar flares can be measured, while a stellar spectrometer would be able to survey hundreds of nearby solar-type stars. This relies upon major advances recently made in transition-edge sensor (TES) detector technology that enable resolution better than 2 eV in an array that can achieve high count rates. Combined with an X-ray mirror, this instrument would combine arcsecond-scale imaging with high- resolution spectra over a modest field of view, enabling a wide range of studies such as the detection of microheating in active regions, ion-resolved velocity flows, and the presence of non-thermal electrons in hot plasmas.
DrRichard MortonUniversity of SheffieldChromospheric jets at the edges of sunspotsRecent results have demonstrated that the chromosphere may play an important role in determining the energetics and dynamics of the corona. While the properties of chromospheric jets are well documented at the limb, in coronal holes and plage regions, details of the jets in and at the boundaries of sunspots are scarce. Using Hinode and TRACE we analyse the properties of jets located at the boundary of a sunspot as it crosses the limb. The jets are seen to continuously raise chromospheric plasma to coronal heights and demonstrate collective behaviour. Enhanced emission at the leading edge of jets suggests the formation of shock fronts leading to heating of the chromospheric plasma. This is supported by emission above the limb observed in the TRACE 1550A and 1600A bandpasses.
DrRyan MilliganQueen s University BelfastSpatially-resolved nonthermal line broadening during the impulsive phase of a solar flareIn this work, which utilises data from the EUV Imaging Spectrometer (EIS) onboard Hinode, broadened line profiles were observed to be co-spatial with two HXR footpoints as observed by RHESSI during the impulsive phase of a C-class flare. By plotting the derived nonthermal velocity for each pixel within the Fe XV and Fe XVI rasters against its corresponding Doppler velocity a strong correlation was found between the two parameters for one of the footpoints. This suggested that the excess broadening at these temperatures is due to a superposition of flows (turbulence), presumably as a result of chromospheric evaporation due to nonthermal electrons. Also presented are diagnostics of electron densities using five pairs of density-sensitive line ratios. Density maps derived using the Mg VII and Si X line pairs showed no appreciable increase in electron density at the footpoints, while the Fe XII, Fe XIII, and Fe XIV line pairs revealed densities approaching 10^11.5 cm −3. Using this information, the nonthermal velocities derived from the widths of the two Fe XIV lines were plotted against their corresponding density values derived from their ratio. This showed that pixels with large nonthermal velocities were associated with pixels of moderately higher densities. This suggests that nonthermal broadening at these temperatures may have been due to enhanced densities at the footpoints, although estimates of the amount of opacity broadening and pressure broadening appeared to be negligible.
DrSarah MatthewsUCL-MSSLChromospheric evaporation, WLFs and SQsSarah Matthews, Sergei Zharkov, Nariaki Nitta Whether WL emission is really common to all flares is likely to be elucidated with the continuous observations now available from SDO, but it remains the case that some M- and X-class flares show surprisingly little emission in the WL, the reasons for which are still unknown. A recent study (Pedram and Matthews (2012)) of the HXR and WL characteristics of WLFs with and without associated sun-quakes  found some evidence for steeper HXR spectra and higher WL contrast in flares with no associated quakes, while Matthews et al (2003) in their survey of Yohkoh WL and non-WL flares found a strong correlation between the incidence of WL emission and high coronal pressure, as well as with the hardness of the HXR spectrum derived from the M2/M1 ratio on HXT. In an attempt to tie these various different observations together we present preliminary results for a flare observed by Hinode, RHESSI, STEREO and SDO in February 2011 in order to study correlations between lower energy electrons, associated chromospheric evaporation, WL contrast and SQs.
DrSergei ZharkovMSSL/UCL
DrSergey ShestovLebedev Physical InstituteEUV spectra of intense solar flares obtained by SPIRIT spectroheliographS. Kuzin We present EUV spectra of several intense solar flares, registered by spectroheliograph SPIRIT aboard Russian CORONAS-F satellite (2001-2005). SPIRIT consisted from two channels ? for the 176-207 and 280- 330 A spectral ranges, each channels was built on a slitless optical scheme with grazing incidence diffraction grating. Field of view of the instrument covered the whole solar disk which allowed us to register several dozens of flares during the satellite lifetime. Identification of spectra, registered by SPIRIT, is complicated by blending of most of the spectral lines, since the instrument had moderate spectral resolution of 0.1 A. We have developed a method for spectra identification to take the blending into account. For each spectrum we apply the following: firstly measure the most intense lines, than in iterative way calculate DEM, calculate synthetic spectrum (using CHAINTI) and fit the experimental spectrum using synthetic one as initial fit. Using synthetic spectrum as initial fit allows one to assess degree of blending and measure intensity of a particular line with a better accuracy. After several iterations (we apply 5 steps which is quite enough) most of the lines in experimental spectrum can be fitted with DEM/synthetic spectrum with accuracy of a factor of 2. In the talk we will discuss features of SPIRIT spectral observation, method details and main results of spectra identification.
MrStefano PucciUniversita` di FirenzeKey Differences between Standard and Blowout Jets in Polar Coronal HolesPucci, S., Poletto, G., Sterling, A.C., Moore, R.L.,Romoli, M. and Bemporad, A.Moore et al. (2010) suggested that polar coronal holes host two kind of jets: standard and blowout. In standard jets an X-ray flaring arcade within the jet base appears offset to one side of the Bright Point arcade; in blowout jets cool material erupts from the flare arcade, making blowout jets and coronal mass ejections share a similar configuration. Examples of jets of the two types have been presented, but an analysis of the physical parameters of these two jet categories has not been done. In this work we examine HINODE/XRT and STEREO/SECCHI observations of a standard jet that occurred in the northern polar coronal hole on July 1, 2008, and of a blowout jet that occurred in the southern polar coronalhole on November 3, 2007, with the aim of identifying the physical parameters of the two events. To this end, we analyzed XRT Al-poly, C-poly, Al-mesh filters mages of the standard jet, Al-poly images of the blowout event and EUVI images of both jets. After illustrating the morphology of the events, we present the results of a filter ratio technique applied to XRT and/or EUVI data, depending on data availability. Temperature profiles along the jet as well as a function of time have been inferred. The standard jet turns out to be cooler than the blowout jet and hardly identifiable in EUVI images while the blowout jet shows up clearly both in XRT and in EUVI 195 and 284 channels. High cadence temperatures have been derived only for the standard jet when multiple XRT filters data are available and do not show an obvious trend over the entire duration of the event. Densities, inferred from Emission Measures, rapidly decrease with distance along the standard jet. An analysis of STEREO/COR1 and SOHO/LASCO C2 images concludes our work.
DrSusanna ParentiRoyal Observatory of BelgiumProminences observations with SDO/AIAS. Parenti, B. Schmieder, P. Heinzel, L. Golub The Prominence-Corona-Transition-Region (PCTR) plays a key role in the thermal and pressure equilibrium of prominences. However, several open issues limit our knowledge of this important interface. Among them we find the thermal structure and the maximum temperature of its emitting plasma. This work is a new step toward resolving these issues. By noting that prominences may be observed in emission in the 171 and 131 SDO/AIA images, while they are seen in absorption in others (e.g. 193) we investigate the temperature content of these channels. Using the CHIANTI atomic database and previously derived prominence DEMs, we built synthetic spectra in these AIA channel to establish the main contributors. We find that the Fe IX line always dominates the 171 band, even in absence of a coronal plasma, while the 131 channel is dominated by Fe VIII. Our conclusion is that the PCTR reaches, at least, 4x10^5 K.
DrTakako KatoNational Institute for Fusion SciencePlasma diagnostics using intensity ratios for plasma dynamics Spectral information is a useful way to know the behavior of plasma especially when we can not directly reach the plasma. Spectral line intensity ratios have been used for plasma diagnostics for temperature and density. In the past we studied He-like iron spectra from solar flares using observations by the ?Hinotori? and ?Yohkoh? satellites. We found a deviation from ionization equilibrium in solar flares. This result is related to the plasma dynamics of the flare. In this paper, we discuss spectra of He-ike C ions measured in the Large Helical Device (LHD) at the National Institute for Fusion Science. The LHD is one of the world?s largest stellarators for fusion research. We studied the time dependent intensity ratios of intercombination lines to the resonance line of He-like C ions. We derived the electron temperatures from the intensity ratios and obtained the position of He-like C ions in plasma. We study the behavior of ions in plasma from the time variation of the position of C ions. It is found that the ionizing state is dominant for He-like C ions even after the energy source is off. These ions are moving towards the hot plasma center after the energy source turns off.
ProfTetsuya WatanabeNational Astronomical Observatory of JapanFeXVII Emission Line Intensity Ratios Seen in EIS and LHD - still the present continuous tense -T. Watanabe (NAOJ), H. Hara (NAOJ), N. Yamamoto (Osaka U.), D. Kato (NIFS), H. A. Sakaue (NIFS), I. Murakami (NIFS) Ne-sequence iron ions, FeXVII, are formed around the temperature of log Te ~ 6.7, which nearly corresponds to the maximum temperature reached in solar active regions. The EIS instrument on board the Hinode mission has detected several week FeXVII emission lines appearing in its observing wavelengths (170 - 210 A, 250 - 290 A), and they are identified as those from the transitions between 2p^5 3s/3p - 2p^5 3p/3d. The observed line intensity ratios among them are compared with our theoretical calculations. Many of them are blended by lower-temperature weak coronal lines, and especially the photon branching ratio of the 2p^5 3p ^3S_0 level to the 2p^5 3s levels has been found wrong by a factor of ~ 2. The intensity ratio of the above two lines have been also measured in the Large Helical Device (LHD) at NIFS (National Institute for Fusion Science) recently, and they are found more or less consistent to the theoretical prediction in our preliminary analysis. We also try to measure these line intensities via a compact/corona EBIT (CoBIT)facility developed at NIFS and ECU (University of Electro-Communications), but we have not been successful so far, although the resonance lines of FeXVII appearing in soft X-ray wavelengths of 15 - 17 A were observed.
DrToshifumi ShimizuISAS/JAXADevelopment of the coronal plasma in an emerging flux regionT. Shimizu, S. Imada, N. Nishizuka (ISAS/JAXA) This talk will present the overall behaviors revealed from EIS, XRT, and SOT observations of an emerging flux region well observed in 29-31 December 2009 and discuss the overall nature of active-region plasma in response to magnetic field development at the solar surface. Sunspots are newly formed with successive emergences of magnetic flux from below the surface (See Shimizu, Ichimoto, Suematsu 2012 ApJ 747 L18 for discovery of an interesting precursory signature of the sunspot penumbra s formation). Chromospheric plasma ejections as well as coronal microflares were frequently produced in response to the evolution of photospheric magnetic fields appeared at the photosphere. We have identified the formation of a magnetic channel formed in the developing sunspot as one of key magnetic field structures for producing coronal microflares and chromospheric ejections frequently. The EIS repeated sparse raster observation provides the temperature structure as well dynamical behaviors (measured as Doppler velocity and line width) with spectral lines including OVI, FeX, FeXII, FeXV and FeXXIII and allows us to discuss observationally how the hot and warm plasma is developed in the active region with occurrence of microflares.
DrUri FeldmanArtep Inc. 2922 Excelsior Spring Court Ellicott City, MD 21042, USACoronal heating - why have we not solved the problem and the kind of spectroscopic measurements that may help resolving itThe talk will explore the reasons of why is it that in spite of six decades of extensive solar physics research, and the launch into space of ever more sophisticate instruments there is still no satisfactory model explaining how solar upper atmosphere plasmas are being created and sustained. When attempts were made to derive such models assumptions were used that although at the time made a lot of sense subsequently where proven wrong. Clearly when such occurred the field suffered setbacks. In the course of the talk observational procedures will be suggested that if implemented could establish reliable facts on which a satisfactory coronal model could be based.
ProfViggo HansteenInstitute of theoretical astrophysics, University of OsloTransition region redshifts and the mass balance of the chromosphere, transition region and corona.In general and on average observations of transition region emission lines reveal the presence of redshifts in lines formed from the top of the chromosphere up to temperatures of about 250000 K and blueshifts for temperatures greater than that. However, it is doubtful that the apparent large downward flows in the lower transition region represent a net flow emptying of the corona, so some mechanism must be responsible for maintaining the mass balance between the lower atmospheric layers and the corona. We use a 3D-MHD code, Bifrost, which includes non-grey, non-LTE radiative transfer in the photosphere and lower chromosphere, optically and effectively thin radiation in the upper chromosphere, transition region and corona, conduction along the magnetic field lines and heating through the ohmic dissipation of tangled magnetic field lines to simulate the solar atmosphere. The motion of material originally in the transition region is tracked as a minority fluid. We report on the coronal mass balance and the mass flow mechanism for conditions perhaps typical of the quiet sun.
DrWardella W. DoschekNone
DrYuan-Kuen KoNaval Research LaboratoryA Study in a Decaying Ephemeral Region on the Correlation of Coronal Properties and Solar Magnetic FieldYuan-Kuen Ko (Naval Research Laboratory), Peter R. Young (George Mason University), Karin Muglach (Artep, Inc.), Enrico Landi (University of Michigan), Uri Feldman (Artep, Inc.) and Harry P. Warren (Naval Research Laboratory) Solar magnetic field is the underlying source that supplies energy to the corona and governs the coronal plasma properties. This work investigates the relationships among coronal properties, namely, the electron temperature, electron density and elemental abundance, and how these coronal properties depend on the strength of the photospheric magnetic field. The data are from observations of a decaying ephemeral region by Hinode/EIS during the course of four days on December 7-11, 2009. We found that there is a positive correlation between Si/S abundance ratio and the electron density/temperature, and the average electron density in this region correlates best with the average unsigned photospheric magnetic field strength.