Fast Magnetosonic Waves and Global Coronal Seismology in the Extended Solar Corona Ryun Young Kwon, Jie Zhang, Maxim Kramar, Tongjiang Wang, Leon Ofman,

Slides:



Advertisements
Similar presentations
Large amplitude transverse oscillations in a multi-stranded EUV prominence centre for fusion, space and astrophysics J. M. Harris C. Foullon, V. M. Nakariakov,
Advertisements

13. Flare Classification in the Era of Global Coverage of the Sun A. Vourlidas, C. Cohen The GOES SXR characterization of solar flares has been used widely.
TRACE and RHESSI observations of the failed eruption of the magnetic flux rope Tomasz Mrozek Astronomical Institute University of Wrocław.
MHD modeling of coronal disturbances related to CME lift-off J. Pomoell 1, R. Vainio 1, S. Pohjolainen 2 1 Department of Physics, University of Helsinki.
Coronal Mass Ejections without photospheric/chromospheric signatures Session organizers: Alexei Pevtsov (NSO) and Vasyl Yurchyshyn (BBSO) Discussion leaders:
Interaction of coronal mass ejections with large-scale structures N. Gopalswamy, S. Yashiro, H. Xie, S. Akiyama, and P. Mäkelä IHY – ISWI Regional meeting.
The Sun’s Dynamic Atmosphere Lecture 15. Guiding Questions 1.What is the temperature and density structure of the Sun’s atmosphere? Does the atmosphere.
Reviewing the Summer School Solar Labs Nicholas Gross.
Strength of Coronal Mass Ejection- driven Shocks Near the Sun and Its Importance in Predicting Solar Energetic Particle Events Chenglong Shen 1, Yuming.
A full view of EIT waves Chen, P.F., Fang, C. & Shibata, K. ApJ, 2005, 622, Solar seminar Shiota.
Electron Acceleration at the Solar Flare Reconnection Outflow Shocks Gottfried Mann, Henry Aurass, and Alexander Warmuth Astrophysikalisches Institut Potsdam,
Coronal Loop Oscillations and Flare Shock Waves H. S. Hudson (UCB/SSL) & A. Warmuth (Astrophysical Institute Potsdam) Coronal loop oscillations: introduction.
Flare waves and the impulsive phase H. S. Hudson Space Sciences Laboratory University of California, Berkeley.
TOWARDS A REALISTIC, DATA-DRIVEN THERMODYNAMIC MHD MODEL OF THE GLOBAL SOLAR CORONA Cooper Downs, Ilia I. Roussev, Bart van der Holst, Noe Lugaz, Igor.
Flare waves and the impulsive phase H. S. Hudson Space Sciences Laboratory University of California, Berkeley.
Soft X-ray observations of global waves Khan-Aurass 2002 Narukage et al Hudson et al
Coronal Loop Oscillations Seen in Unprecedented Detail by SDO/AIA Rebecca White and Erwin Verwichte University of Warwick, Centre for Fusion, Space and.
CME-driven Shocks in White Light Observations SOHO/LASCO C3 – CME May 5 th, 1999 CME-driven Shock We demonstrate that CME-driven shocks: (1) can be detected.
Tucson MURI SEP Workshop March 2003 Janet Luhmann and the Solar CISM Modeling Team Solar and Interplanetary Modeling.
Reconstructing Active Region Thermodynamics Loraine Lundquist Joint MURI Meeting Dec. 5, 2002.
IGPP, March Coronal shock waves observed in images H.S. Hudson SSL/UCB.
Glasgow, March 24, 2005 Large-scale coronal shock waves H.S. Hudson SSL/UCB.
Coronal Loop Oscillations and Flare Shock Waves H. S. Hudson (UCB/SSL) & A. Warmuth (Astrophysical Institute Potsdam) Coronal loop oscillations: (Fig.
Paper Review Special Issue of Solar Physics (I) STEREO Science Results at Solar Minimum Volume 259, Numbers 1-2 / October 2009 Yan Xu 2010 Nov. 02.
Waves and Currents in Coronal Active Regions Leon Ofman* Catholic University of America NASA Goddard Space Flight Center *Visiting, Tel Aviv University.
Coronal waves: hot structure and footprint of CME.
Flare energy and fast electrons via Alfvén waves H. S. Hudson & L. Fletcher SSL/Berkeley and Glasgow U.
Solar Origin of energetic particle events Near-relativistic impulsive electron events observed at 1 AU M. Pick, D. Maia, S.J. Wang, A. Lecacheux, D. Haggery,
Overview of White Light & Radio Signatures of CMEs Angelos Vourlidas Naval Research Laboratory.
Observing the Sun. Corona: EUV; X-rays Chromosphere: H , UV, EUV Photosphere: near UV, Visible light, infra-red.
Pietro Zucca, Eoin Carley, Shaun Bloomfield, Peter Gallagher
High-Cadence EUV Imaging, Radio, and In-Situ Observations of Coronal Shocks and Energetic Particles: Implications for Particle Acceleration K. A. Kozarev.
Shock wave formation heights using 2D density and Alfvén maps of the corona ABSTRACT Coronal shock waves can produce decametric radio emission known Type.
The Sun and the Heliosphere: some basic concepts…
Relation between Type II Bursts and CMEs Inferred from STEREO Observations N. Gopalswamy, W. Thompson, J. Davila, M. Kaiser NASA Goddard Space Flight Center,
1 THE RELATION BETWEEN CORONAL EIT WAVE AND MAGNETIC CONFIGURATION Speakers: Xin Chen
195 Å image – behind 195 Å image – Sun- Earth line – SOHO/ EIT image 195 Å image – Sun- Earth line – SOHO/ EIT image 195 Å image – ahead SECCHI Extreme.
Observations of Moreton waves with Solar-B NARUKAGE Noriyuki Department of Astronomy, Kyoto Univ / Kwasan and Hida Observatories M2 The 4 th Solar-B Science.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Heliosphere: The Solar Wind March 01, 2012.
Flare-associated shock waves observed in soft X-ray NARUKAGE Noriyuki Kwasan and Hida Observatories, Kyoto University – DC3 The 6 th Solar-B Science Meeting.
A multiwavelength study of solar flare waves II. Perturbation characteristics and physical interpretation A. Warmuth, B. Vrsnak, J. Magdalenic, A. Hanslmeier,
Deconstructing EIT Waves Marco Velli Jet Propulsion Laboratory, Caltech and Dipartimento di Astronomia e Scienza dello Spazio, Università di Firenze Thompson.
34th Solar Physics Division Meeting, June 2003 Propagating Disturbances in the Lower Solar Corona Meredith J. Wills-Davey Southwest Research Institute.
Flare-Associated Oscillations Observed with NoRH Ayumi Asai (NSRO) Nobeyama Symposium 2004 : 2004/10/26.
IMAGING AND SPECTOROPIC INVESTIGATIONS OF A SOLAR CORONAL WAVE: PROPERTIES OF THE WAVE FRONT AND ASSOCIATED ERUPTING MATERIAL L OUISE K. HARRA AND A LPHONSE.
A Numerical Study of the Breakout Model for Coronal Mass Ejection Initiation P. MacNeice, S.K. Antiochos, A. Phillips, D.S. Spicer, C.R. DeVore, and K.
Shock heating by Fast/Slow MHD waves along plasma loops
ISSI, Beijing, China. The famous example of the decaying kink oscillations of coronal loops observed with the TRACE ISSI, Beijing,
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Fall, 2009 Copyright © The Heliosphere: Solar Wind Oct. 08, 2009.
Analysis of 3 and 8 April 2010 Coronal Mass Ejections and their Influence on the Earth Magnetic Field Marilena Mierla and SECCHI teams at ROB, USO and.
Review: Recent Observations on Wave Heating S. Kamio Kwasan and Hida Observatories Kyoto University.
Three-Dimensional Structure of Coronal Mass Ejections From LASCO Polarization Measurements K. P. Dere, D. Wang and R. Howard ApJL, 620; L119-L
Global coronal seismology and EIT waves Istvan Ballai SP 2 RC, University of Sheffield, UK.
Relationships between flares and CMEs FRIDAY 9:00 am – 12:00 pm SHINE 2009.
Interplanetary proton and electron enhancements associated with radio-loud and radio-quiet CME-driven shocks P. Mäkelä 1,2, N. Gopalswamy 2, H. Xie 1,2,
Coronal Seismology Based on EUV Waves P. F. Chen , China.
CME-driven Shocks in White Light Observations Verónica Ontiveros National University of Mexico, MEXICO George Mason University,USA Angelos Vourlidas Naval.
An Introduction to Observing Coronal Mass Ejections
Marina Battaglia, FHNW Säm Krucker, FHNW/UC Berkeley
Particle Acceleration at Coronal Shocks: the Effect of Large-scale Streamer-like Magnetic Field Structures Fan Guo (Los Alamos National Lab), Xiangliang.
N. Gopalswamy, H. Xie, S. Akiyama, P. Mäkelä, S. Yashiro, I. Usoskin
Exploring Large-scale Coronal Magnetic Field Over Extended Longitudes With EUVI EUVI B EIT EUVI A 23-Mar UT Nariaki Nitta, Marc DeRosa, Jean-Pierre.
Difficult to relate EIT waves to other phenomena due to cadence
Series of high-frequency slowly drifting structure mapping the magnetic field reconnection M. Karlicky, A&A, 2004, 417,325.
Solar Sources of Wide Coronal Mass Ejections during the Ascending Phase of Cycle 24 Sachiko Akiyama1,2, Nat Gopalswamy2, Seiji Yashiro1,2 , and Pertti.
High-cadence Radio Observations of an EIT Wave
Flare-Associated Oscillations Observed with NoRH
Magnetic connection between the photosphere and the corona
On the nature of EIT waves, EUV dimmings and their link to CMEs
Sakai, J. I., Nishi, K., and Sokolov, I. V. ApJ, 2002, 576, 1018
Presentation transcript:

Fast Magnetosonic Waves and Global Coronal Seismology in the Extended Solar Corona Ryun Young Kwon, Jie Zhang, Maxim Kramar, Tongjiang Wang, Leon Ofman, & Joseph M. Davila

Contents Finding: Fast magnetosonic waves in the extended solar corona Application: Global coronal seismology I wanna show today global coronal seismology, to determine magnetic field strengths in the extended solar corona, using traveling fast magnetosonic waves. My talk consists of two parts. The first, I’m gonna introduce new observations of fast magnetosonic waves, traveling in the extended solar corona, observed by STEREO COR1 coronagraphs. And I’m gonna prove that the traveling disturbance is in fact fast magnetosonic waves. Than, I’ll discuss the results.

Introduction Fast magnetosonic waves associated with flares/CMEs Moreton waves (Moreton 1960), EUV waves (Thompson et al. 1999), and type II radio bursts (Wagner & MacQueen 1983) Reasons for controversies: unknown physical parameters, especially, magnetic field strengths -> local fast mode (Alfvén) speed Previous coronal seismology Localized magnetic structures (e.g., coronal loops; Aschwanden et al. 1999) A specific coronal layer (e.g., EUV wave; Ballai 2007) Radial or nearly radial direction (e.g., type II radio burst and shock ahead of CME leading edge; Vršnak et al. 2002; Gopalswamy & Yashiro 2011) PFSS models: Neglected plasma structures. Global coronal seismology in the extended solar corona for comprehensive understanding of various aspects of fast magnetosonic waves Associated with flares/CMEs, fast magnetosonic waves may be triggered to propagate into the solar coronal medium and they may be observed in the form of Moreton waves, EUV waves, and type II radio bursts. However, it has been highly debated whether or not that they are truly fast magnetosonic waves. The most important reason for … we have no idea what’s going on in the corona. In order to overcome… Note that the fast mode waves are global phenomena, traveling across magnetized plasma structures. So, in order to interpret the observed signatures of fast mode waves, we should understand global distributions of magnetic field strengths.

Fast magnetosonic wave vs. Magnetic reconguration scenario Imaging observations of coronal fast magnetosonic waves: EUV waves The first thing, we have to find true waves to apply for global coronal seismology. I wanna remind you there is a still a debate on the nature of EUV waves. In general, it’s hard to know whether or not that the observed fronts are true wave fronts or not. This movies show EUV waves observed by two STEREO spacecrafts, supporting that the EUV waves are in fact fast mode waves  Patsourakos &Vourlidas, Angelos 2009

Alternative interpretation (Schrijver et al. 2011) There exists an alternative interpretations. They pointed out that the global magnetic field configuration is very imporant. It can be observed a freely propagating front separated from CME body. These scenarios are highly supported by an observational characteristics of EUV waves, this is stationary fronts. It is well know that propagating EUV waves stop.. Separation from flux rope (current shell or overlying magnetic field lines) Stop at separatrices (boundaries of coronal holes) -> stationary fronts Constraint: Streamers (global separatrices)

White-light wave Kwon et al. (2013, ApJ, 766, 55)

Time-distance maps

Global coronal seismology Fast magnetosonic speed, Alfvén speed, Sound sped, Magnetic field are parallel to each other and wave vectors are perpendicular to the magnetic field lines, Magnetic field strength in cgs unit,

Radial profiles Speeds of white light wave are in fact local fast magnetosonic speeds! Saito et al. (1977)

Physical implications: EUV waves EUV waves would be refracted toward upper corona or lower chromosphere corona and disappear. http://en.wikipedia.org/wiki/Seismology

Side view Top view Low coronal layer EIT waves are signatures of downward fast magnetosonic waves refracted from the upper solar corona, as the same as an interpretation of Moreton waves (Uchida 1968), rather than freely propagating fast magnetosonic wave in a certain coronal layer.

Physical Implications Correlation between fast magnetosonic speed and magnetic field strength Yang & Chen (2010) found that speeds of EUV waves have significant negative correlation with magnetic field strengths determined with a potential field model. Correlation coefficients of fast magnetosonic speed Electron density (ne-1/2): 0.61 Magnetic field strength: -0.02 Electron density is important! (not modeled magnetic field) Discrepancy of speeds between EUV waves and type II radio bursts (Klassen et al. 2000) Increasing fast magnetosonic speed with height: 465km s−1 (EUV wave), 829 to 1723 km s−1 (White light wave at 1.6 – 3.0 Rs) Type II radio bursts are shock signatures in the upper corona

Summary High time cadence white-light observations: STEREO SECCHI COR1 coronagraphs White light waves Global coronal seismology (magnetic field strengths in a wide spatial range of the extended solar corona) Interpretations of various manifestations of fast magnetosonic waves Moreton waves and EUV waves EUV waves vs. type II radio bursts

Thank you!!