Waves and Oscillations in the Solar Corona First Year Progress Report
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Coronal Structure of Pre-Main Sequence Stars
**FULL TITLE** ASP Conference Series, Vol. **VOLUME**, **YEAR OF PUBLICATION** **NAMES OF EDITORS** Coronal Structure of Pre-Main Sequence Stars Moira Jardine SUPA, School of Physics and Astronomy, North Haugh, St Andrews, Fife, KY16 9SS, UK Abstract. The study of pre-main sequence stellar coronae is undertaken in many different wavelength regimes, with apparently conflicting results. X-ray studies of T Tauri stars suggest the presence of loops with a range of sizes ranging from less than a stellar radius to 10 stellar radii. Some of these stars show a clear rotational modulation in X-rays, but many do not and indeed the nature of this emission and its dependence on stellar mass and rotation rate is still a matter of debate. Some component of it may come from the accretion shock, but the location and extent of the accretion funnels (inferred from optical and UV observations) is as much of a puzzle as the mass accretion rate that they carry. Mass and angular momentum are not only gained by the star in the process of accretion, but also lost in either jets or winds. Linking all these different features is the magnetic field. Recent observations suggest the presence of structure on many scales, with a complex, multipolar field on small scales near the surface co-existing with a much simpler field structure on the larger scales at which the stellar field may be linking onto a surrounding disk. Some recent models suggest that the open field lines which are responsible for carrying gas escaping in winds and jets may also be responsible for much of the infalling accretion flow. -
15 Stellar Winds
15 Stellar Winds Stan Owocki Bartol Research Institute, Department of Physics and Astronomy, University of Colorado, Newark, DE, USA 1IntroductionandBackground....................................... 737 2ObservationalDiagnosticsandInferredProperties....................... 740 2.1 Solar Corona and Wind ................................................ 740 2.2 Spectral Signatures of Dense Winds from Hot and Cool Stars ................. 742 2.2.1 Opacity and Optical Depth ............................................. 742 2.2.2 Doppler-Shi!ed Line Absorption ........................................ 744 2.2.3 Asymmetric P-Cygni Pro"les from Scattering Lines ......................... 745 2.2.4 Wind-Emission Lines .................................................. 748 2.2.5 Continuum Emission in Radio and Infrared ................................ 750 3GeneralEquationsandFormalismforStellarWindMassLoss.............. 751 3.1 Hydrostatic Equilibrium in the Atmospheric Base of Any Wind ............... 751 3.2 General Flow Conservation Equations .................................... 752 3.3 Steady, Spherically Symmetric Wind Expansion ............................ 753 3.4 Energy Requirements of a Spherical Wind Out#ow .......................... 753 4CoronalExpansionandSolarWind................................... 754 4.1 Reasons for Hot, Extended Corona ....................................... 754 4.1.1 $ermal Runaway from Density and Temperature Decline of Line-Cooling ...... 754 4.1.2 Coronal Heating with a Conductive $ermostat ........................... -
The High Resolution Camera
CXC Newsletter The High Resolution Camera To create a source catalog of the M31 center and search for time variability of the sources, we includ- Ralph Kraft, Hans Moritz Guenther (SAO), and ed 23 observations from November 1999 to February Wolfgang Pietsch (MPE) 2005 (adding about 250 ks exposure time). We detected 318 X-ray sources and created long term light curves It has been another quiet, but successful year for for all of them. We classified sources as highly variable HRC operations. The instrument performs well with or outbursting (with subclasses short vs. long outbursts no significant anomalies or instrumental issues. The and activity periods). 129 sources could be classified as HRC continues to be used for a wide variety of astro- X-ray binaries due to their position in globular clusters physical investigations. In this chapter, we briefly de- or their strong time variability (see Fig. 2). We detected scribe two such science studies. First, a collaboration seven supernova remnants, one of which is a new can- led by Dr. Wolfgang Pietsch of MPE used the HRC to didate, and also resolved the first X-rays from a known study the X-ray state of the nova population in M31 radio supernova remnant (see Hofmann et al. 2013). in conjunction with XMM-Newton and optical studies. In a second study, Guenther et al. used the HRC to They found that there is a strong correlation between determine the origin of the X-ray emission from β Pic, the optical and X-ray properties of these novae. Sec- a nearby star with a dusty disk. -
1 Introduction
1 1 Introduction Uchida [1], who suggested the idea of plasma and magnetic field diagnostics in the solar corona on the basis of waves and oscillations in 1970, and Rosenberg [2], who first explained the pulsations in type IV solar radio bursts in terms of the loop magnetohydrodynamic (MHD) oscillations, can be considered to be pioneers of coronal seismology. Various approaches have been used to describe physical processes in stellar coronal structures: kinetic, MHD, and electric circuit models are among them. Two main models are presently very popular in coronal seismology. The first considers magnetic flux tubes and loops as wave guides and resonators for MHD waves and oscillations, whereas the second describes a loop in terms of an equivalent electric (RLC) circuit. Several detailed reviews are devoted to problems of coronal seismology (see, i.e., [3–7]). Recent achievements in the solar coronal seismology are also referred in Space Sci. Rev. vol. 149, No. 1–4 (2009). Nevertheless, some important issues related to diagnostics of physical processes and plasma parameters in solar and stellar flares are still insufficiently presented in the literature. The main goal of the book is the successive description and analysis of the main achievements and problems of coronal seismology. There is much in common between flares on the Sun and on late-type stars, especially red dwarfs [8]. Indeed, the timescales, the Neupert effect, the fine structure of the optical, radio, and X-ray emission, and the pulsations are similar for both solar and stellar flares. Studies of many hundreds of stellar flares have indicated that the latter display a power–law radiation energy distribution, similar to that found for solar flares. -
Variability of a Stellar Corona on a Time Scale of Days Evidence for Abundance Fractionation in an Emerging Coronal Active Region
A&A 550, A22 (2013) Astronomy DOI: 10.1051/0004-6361/201220491 & c ESO 2013 Astrophysics Variability of a stellar corona on a time scale of days Evidence for abundance fractionation in an emerging coronal active region R. Nordon1,2,E.Behar3, and S. A. Drake4 1 Max-Planck-Institut für Extraterrestrische Physik (MPE), Postfach 1312 85741 Garching, Germany 2 School of Physics and Astronomy, The Raymond and Beverly Sackler Faculty of Exact Sciences, Tel-Aviv University, 69978 Tel-Aviv, Israel e-mail: [email protected] 3 Physics Department, Technion Israel Institute of Technology, 32000 Haifa, Israel e-mail: [email protected] 4 NASA/GSFC, Greenbelt, 20771 Maryland, USA e-mail: [email protected] Received 3 October 2012 / Accepted 1 December 2012 ABSTRACT Elemental abundance effects in active coronae have eluded our understanding for almost three decades, since the discovery of the first ionization potential (FIP) effect on the sun. The goal of this paper is to monitor the same coronal structures over a time interval of six days and resolve active regions on a stellar corona through rotational modulation. We report on four iso-phase X-ray spectroscopic observations of the RS CVn binary EI Eri with XMM-Newton, carried out approximately every two days, to match the rotation period of EI Eri. We present an analysis of the thermal and chemical structure of the EI Eri corona as it evolves over the six days. Although the corona is rather steady in its temperature distribution, the emission measure and FIP bias both vary and seem to be correlated. -
“Oscillatory Processes in Solar and Stellar Coronae”
www.issibj.ac.cn ISSI-BJ WORKSHOP “OSCILLATORY PROCESSES IN SOLAR AND STELLAR CORONAE” Topics I. Sergey Anfinogentov, et al. "Novel techniques in coronal seismology data analysis" II. Valery Nakariakov, et al. "Kink oscillations and waves in the corona" III. Tongjiang Wang, et al. "Slow waves in coronal loops" IV. Dipankar Banerjee, et al. "MHD waves in open coronal structures" V. Ivan Zimovets, et al. "Quasi-periodic pulsations in solar and stellar flares" VI. Bo Li, et al. "Sausage oscillations and waves in the corona" VII. Tom Van Doorsselaere, et al. "Coronal heating by MHD waves” VIII. Other I. Sergey Anfinogentov, et al. "Novel techniques in coronal seismology data analysis" David Pascoe High-resolution Diagnostic Techniques for the Solar Corona The high spatial and temporal resolution provided by the Atmospheric Imaging Assembly of the Solar Dynamics Observatory has inspired the development of advanced observational techniques to probe the solar atmosphere. For example, forward modelling of the EUV intensity of coronal structures and the seismological analysis of kink oscillations provide powerful diagnostics to constrain properties such as the plasma density and magnetic field strength. We also increasingly employ Bayesian analysis and Markov chain Monte Carlo sampling in our analysis to increase the robustness and accuracy of our modelling. These techniques are now also being applied to study quasi-periodic pulsations associated with solar and stellar flares. [email protected] www.issibj.ac.cn Inigo Arregui Recent results in Bayesian coronal and prominence seismology We report on recent results from the application of Bayesian analysis techniques to seismology of coronal loops and prominence fine structures. -
19910023712.Pdf
SOLAR ASTRONOMY IX-1 Solar Astronomy 59-el N91-38026 Table of Contents 0. Executive Summary ................................ page 2 1. An Overview of Modern Solar Physics ......................... page 5 1.1 General Perspectives .............................. page 5 1.2 Frontiers and Goals for the 1990s ........................ page 8 1.2.1 The Solar Interior ............................ page 8 1.2.2 The Solar Surface ............................ page 9 1.2.3 The Outer Solar Atmosphere: Corona and Heliosphere ............ page 9 1.2.4 The Solar-Stellar Connection ....................... page 10 2. Ground-Based Solar Physics ............................. page 11 2.1 Introduction ................................. page 11 2.2 Status of Major Projects and Facilities ...................... page 11 2.3 A Prioritized Ground-based Program for the 1990s ................. page 12 2.3.1 Prerequisites .............................. page 12 2.3.2 Prioritization .............................. page 12 2.3.3 The Major Initiative: Solar Magnetohydrodynamics, and the LEST ....... page 12 2.3.3.1 The Large Earth-based Solar Telescope (LEST) ............ page 14 2.3.3.2 Infrared Facility Development .................... page 15 2.3.4 Moderate Initiatives ........................... page 15 2.3.5 Interdisciplinary Initiatives ........................ page 18 2.4 Conclusions and Summary ........................... page 20 3. Space Observations For Solar Physics ......................... page 20 3.1 Introduction ................................. page 20 3.2 -
Temporal Evolution of Mhd Waves in Solar Coronal Arcades
DOCTORAL THESIS 2019 TEMPORAL EVOLUTION OF MHD WAVES IN SOLAR CORONAL ARCADES Samuel Rial Lesaga palabra DOCTORAL THESIS 2019 Doctoral Programe of Physics TEMPORAL EVOLUTION OF MHD WAVES IN SOLAR CORONAL ARCADES. Samuel Rial Lesaga Thesis supervisor: I~nigoArregui Uribe-Echevarria Thesis supervisor: Ram´onOliver Herrero Thesis Tutor: Alicia Sintes Olives Doctor by the university of the Balearic islands Supervisor letter Supervisor letter v Supervisor letter Supervisor letter Dr. I˜nigo Arregui Uribe-Echebarria of the Instituto de Astrof´ısica de Canarias. DECLARE: That the thesis entitled “Temporal evolution of magnetohydrodynamic waves in solar coronal arcades”, presented by Samuel Rial Lesaga to obtain the PhD degree, has been completed under my supervision. For all intents and purposes, I hereby sign this document. Signature Firmado por ARREGUI URIBE- ECHEVARRIA IÑIGO - 15392542E el día 20/05/2019 con un certificado emitido por AC FNMT Usuarios Dr. I˜nigo Arregui Uribe-Echebarria La Laguna, 17 May 2019 vi Acknowledgments En primer lugar me gustar´ıaagradecer al Dr. Ramon Oliver la amistad, la con- fianza y el apoyo incondicional que me siempre me ha ofrecido. El siempre ha sabido animarme y motivarme en los m´ultiplesmomentos dif´ıcilesque ha tenido esta tesis y estoy plenamente convencido de que si no hubiera sido por ´elesta tesis no existir´ıa. Gracias Al Dr. I~nigoArregui por su paciencia y su confianza en mi trabajo y en mi. Gracias motivarme cuando no lo estaba y por hacerme ver que este esfuerzo merece la pena. Al Dr. Jos´eLuis Ballester y a todo el grupo de personas que forman o han formado parte el grupo de f´ısicasolar de la Universitat de les Illes Balears y con los que he compartido alg´uncongreso, desayuno o cena. -
Measuring the Density Structure of an Accretion Hot Spot
Article Measuring the density structure of an accretion hot spot https://doi.org/10.1038/s41586-021-03751-5 C. C. Espaillat1 ✉, C. E. Robinson2, M. M. Romanova3, T. Thanathibodee4, J. Wendeborn1, N. Calvet4, M. Reynolds4 & J. Muzerolle5 Received: 4 March 2021 Accepted: 21 June 2021 Magnetospheric accretion models predict that matter from protoplanetary disks Published online: 1 September 2021 accretes onto stars via funnel fows, which follow stellar magnetic feld lines and shock Open access on the stellar surfaces1–3, leaving hot spots with density gradients4–6. Previous work Check for updates has provided observational evidence of varying density in hot spots7, but these observations were not sensitive to the radial density distribution. Attempts have been made to measure this distribution using X-ray observations8–10; however, X-ray emission traces only a fraction of the hot spot11,12 and also coronal emission13,14. Here we report periodic ultraviolet and optical light curves of the accreting star GM Aurigae, which have a time lag of about one day between their peaks. The periodicity arises because the source of the ultraviolet and optical emission moves into and out of view as it rotates along with the star. The time lag indicates a diference in the spatial distribution of ultraviolet and optical brightness over the stellar surface. Within the framework of a magnetospheric accretion model, this fnding indicates the presence of a radial density gradient in a hot spot on the stellar surface, because regions of the hot spot with diferent densities have diferent temperatures and therefore emit radiation at diferent wavelengths. -
Coronal Seismology Through Wavelet Analysis
A&A 381, 311–323 (2002) Astronomy DOI: 10.1051/0004-6361:20011659 & c ESO 2002 Astrophysics Coronal seismology through wavelet analysis I. De Moortel1,A.W.Hood1, and J. Ireland2 1 School of Mathematics and Statistics, University of St Andrews, North Haugh, St Andrews, Fife KY16 9SS, UK 2 Osservatorio Astronomica de Capodimonte, via Moiariello 16, 80131 Napoli, Italy Received 10 September 2001 / Accepted 18 October 2001 Abstract. This paper expands on the suggestion of De Moortel & Hood (2000) that it will be possible to infer coronal plasma properties by making a detailed study of the wavelet transform of observed oscillations. TRACE observations, taken on 14 July 1998, of a flare-excited, decaying coronal loop oscillation are used to illustrate the possible applications of wavelet analysis. It is found that a decay exponent n ≈ 2 gives the best fit to the 2 double logarithm of the wavelet power, thus suggesting an e−εt damping profile for the observed oscillation. Additional examples of transversal loop oscillations, observed by TRACE on 25 October 1999 and 21 March 2001, n are analysed and a damping profile of the form e−εt ,withn ≈ 0.5andn ≈ 3 respectively, is suggested. It is n demonstrated that an e−εt damping profile of a decaying oscillation survives the wavelet transform, and that the value of both the decay coefficient ε and the exponent n can be extracted by taking a double logarithm of the normalised wavelet power at a given scale. By calculating the wavelet power analytically, it is shown that a sufficient number of oscillations have to be present in the analysed time series to be able to extract the period of the time series and to determine correct values for both the damping coefficient and the decay exponent from the wavelet transform. -
FROM SOLAR to STELLAR CORONA: the ROLE of WIND, ROTATION, and MAGNETISM Victor Réville1, Allan Sacha Brun1, Antoine Strugarek1,2, Sean P
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Open Research Exeter The Astrophysical Journal, 814:99 (9pp), 2015 December 1 doi:10.1088/0004-637X/814/2/99 © 2015. The American Astronomical Society. All rights reserved. FROM SOLAR TO STELLAR CORONA: THE ROLE OF WIND, ROTATION, AND MAGNETISM Victor Réville1, Allan Sacha Brun1, Antoine Strugarek1,2, Sean P. Matt3, Jérôme Bouvier4, Colin P. Folsom4, and Pascal Petit5 1 Laboratoire AIM, DSM/IRFU/SAp, CEA Saclay, F-91191 Gif-sur-Yvette Cedex, France; [email protected], [email protected] 2 Département de physique, Université de Montréal, C.P. 6128 Succ. Centre-Ville, Montréal, QC H3C 3J7, Canada; [email protected] 3 Department of Physics and Astronomy, University of Exeter, Stocker Road, Exeter EX4 4SB, UK; [email protected] 4 IPAG, Université Joseph Fourier, B.P.53, F-38041 Grenoble Cedex 9, France; [email protected], [email protected] 5 IRAP, CNRS—Université de Toulouse, 14 avenue Edouard Belin, F-31400 Toulouse, France; [email protected] Received 2015 July 6; accepted 2015 September 21; published 2015 November 20 ABSTRACT Observations of surface magnetic fields are now within reach for many stellar types thanks to the development of Zeeman–Doppler Imaging. These observations are extremely useful for constraining rotational evolution models of stars, as well as for characterizing the generation of the magnetic field. We recently demonstrated that the impact of coronal magnetic field topology on the rotational braking of a star can be parameterized with a scalar parameter: the open magnetic flux. -
Coronal Magnetic Field Measurement Using Loop Oscillations Observed by Hinode/EIS
A&A 487, L17–L20 (2008) Astronomy DOI: 10.1051/0004-6361:200810186 & c ESO 2008 Astrophysics Letter to the Editor Coronal magnetic field measurement using loop oscillations observed by Hinode/EIS T. Van Doorsselaere1,V.M.Nakariakov1, P. R. Young2, and E. Verwichte1 1 Centre for Fusion, Space and Astrophysics, Physics Department, University of Warwick, Coventry CV4 7AL, UK e-mail: [t.van-doorsselaere;v.nakariakov;erwin.verwichte]@warwick.ac.uk 2 STFC, Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire OX11 0QX, UK e-mail: [email protected] Received 13 May 2008 / Accepted 12 June 2008 ABSTRACT We report the first spectroscopic detection of a kink MHD oscillation of a solar coronal structure by the Extreme-Ultraviolet Imaging Spectrometer (EIS) on the Japanese Hinode satellite. The detected oscillation has an amplitude of 1 km s−1 in the Doppler shift of the FeXII 195 Å spectral line (1.3 MK), and a period of 296 s. The unique combination of EIS’s spectroscopic and imaging abilities enables us to measure simultaneously the mass density and length of the oscillating loop. This enables us to measure directly the magnitude of the local magnetic field, the fundamental coronal plasma parameter, as 39 ± 8 G, with unprecedented accuracy. This proof of concept makes EIS an exclusive instrument for the full scale implementation of the MHD coronal seismological technique. Key words. instrumentation: spectrographs – Sun: corona – Sun: oscillations – Sun: magnetic fields 1. Introduction oscillating structure. In the case of standing waves, the phase speed can be estimated by the period of the observed oscilla- Coronal seismology utilises observed waves and oscillations in tions and the wavelength given by the size of the resonator.