Observation of Sigmoids with Solar-B

Slides:



Advertisements
Similar presentations
The flare-CME relationship – determining factors (if any!) Sarah Matthews, Lucie Green, Hilary Magee, Louise Harra & Len Culhane MSSL, University College.
Advertisements

The 3D picture of a flare Loukas Vlahos. Points for discussion  When cartoons drive the analysis of the data and the simulations….life becomes very complicated.
The magnetic nature of solar flares Paper by E.R. Priest & T.G. Forbes Review presented by Hui Song.
Estimating the magnetic energy in solar magnetic configurations Stéphane Régnier Reconnection seminar on Thursday 15 December 2005.
Energy and Helicity Budget of Four Solar Flares and Associated Magnetic Clouds. Maria D. Kazachenko, Richard C. Canfield, Dana Longcope, Jiong Qiu Montana.
Study of Magnetic Helicity Injection in the Active Region NOAA Associated with the X-class Flare of 2011 February 15 Sung-Hong Park 1, K. Cho 1,
1. Helicity: basic properties, open geometries 2. Observations of helicity and helicity flux 3. Twist and Writhe Mitchell Berger Review of Magnetic Helicity.
Sarah Gibson October 2005 Twisted magnetic flux ropes: A breeding ground for CMEs? Sarah Gibson Collaborators: Yuhong Fan, Joan Burkepile, Giuliana de.
A flare compilation Lots of people including Louise Harra, Lidia van Driel Gesztelyi, Chris Goff, Sarah Matthews, Len Culhane, Cristina Mandrini, Pascal.
1 Hinode Coordinated Observations: Plasma Composition Photospheric composition ~ 1 in coronal hole (CH) -> fast wind Coronal composition ~1.5-3 in active.
Coronal Mass Ejections without photospheric/chromospheric signatures Session organizers: Alexei Pevtsov (NSO) and Vasyl Yurchyshyn (BBSO) Discussion leaders:
TRACE Downflows and Energy Release Ayumi ASAI Kwasan Observatory, Kyoto University Magnetic Reconnection and the Dynamic Sun 9 September, Andrews.
The Hemispheric Pattern of Filaments and Consequences for Filament Formation Duncan H Mackay Solar Physics Group University of St. Andrews.
Active Region Evolution and the Removal of Magnetic Helicity by CMEs Len Culhane Mullard Space Science Laboratory University College London.
Sigmoidal Active Regions on the Sun: Statistical and Detailed Studies Lily Hanson Advisors: Ed DeLuca and Antonia Savcheva
The Relation between Filament Skew Angle and Magnetic Helicity of Active Regions Masaoki HAGINO, Y.J. MOON (Korea Astronomy and Space Science Institute)
STEREO AND SPACE WEATHER Variable conditions in space that can have adverse effects on human life and society Space Weather: Variable conditions in space.
What can helicity redistribution in solar eruptions tell us about reconnection in these events? by Brian Welsch, JSPS Fellow (Short-Term ), Space Sciences.
Chip Manchester 1, Fang Fang 1, Bart van der Holst 1, Bill Abbett 2 (1)University of Michigan (2)University of California Berkeley Study of Flux Emergence:
SHINE Campaign Event: 1-2 May 1998 Brian Welsch (& Yan Li) Space Sciences Laboratory, UC Berkeley Introduction: Data, Context, etc. Work: Completed & Ongoing.
Jonathan A. Constable University of St Andrews Solar REU Presentation 2009 A flux rope model for CME initiation over solar cycle 23 Jonathan Constable.
SHINE The Role of Sub-Surface Processes in the Formation of Coronal Magnetic Flux Ropes A. A. van Ballegooijen Smithsonian Astrophysical Observatory.
MSU Team: R. C. Canfield, D. W. Longcope, P. C. H. Martens, S. Régnier Evolution on the photosphere: magnetic and velocity fields 3D coronal magnetic fields.
Understanding Magnetic Eruptions on the Sun and their Interplanetary Consequences A Solar and Heliospheric Research grant funded by the DoD MURI program.
Discussion Group B: Progress on Initiation Mechanisms 1. Determine topology of initiating field –Initiate broad observational investigation on filament.
Observations of the failed eruption of the magnetic flux rope – a direct application of the quadrupolar model for a solar flare Tomasz Mrozek Astronomical.
FLUX CANCELLATION IN PROMINENCE FORMATION Piet Martens Montana State University, Bozeman, MT, USA & Paul Wood University of St Andrews, Fife, Scotland.
Some Thoughts on Transients: Buildup & Release of Energy David E. McKenzie, Montana State University—Bozeman HMI/AIA Science Team MeetingMonterey, February.
Solar-B XRT XRT-1 The Science and Capability of the Solar-B / X-Ray Telescope Solar-B XRT Presenter: Ed DeLuca Smithsonian Astrophysical Observatory.
Center for Space Environment Modeling Ward Manchester University of Michigan Yuhong Fan High Altitude Observatory SHINE July.
Coronal Mass Ejections: Models and Their Observational Basis (P.F. Chen Living Rev. Solar Phys.) 张英智 中国科学院空间科学与应用研究中心空间天气学国家重点实验室.
Working Group E: The Pre-CME Sun - Pre-eruption structure, evolution & energy release - Global issues: helicity, homologous CMEs - Inputs to CME initiation.
Solar-B Science Objectives - Overview of the Mission - Kazunari Shibata (Kyoto Univ.)
Kinetic and Magnetic Helicities of Solar Active Regions Ram Ajor Maurya, Ashok Ambastha And Vema Reddy Udaipur Solar Observatory Physical Research Laboratory,
EUV vs. B-field Comparisons Yingna Su Smithsonian Astrophysical Observatory Coauthours: Leon Golub, Aad Van Ballegooijen, Maurice Gros. HMI/AIA Science.
Photospheric Sources of Very Fast (>1100km/s) Coronal Mass Ejections Recent studies show that only very fast CMEs (> 1100 km/s) are capable of producing.
Direct Evidence of Emergence of a Helical Flux Rope under an Active- Region Prominence Joten Okamoto Kyoto Univ. / NAOJ JSPS Research Fellow Saku Tsuneta,
Magnetic Structures of Active Regions and their Link to Coronal Mass Ejections Vasyl Yurchyshyn, Big Bear Solar Observatory, Big Bear City, CA 92314,
Twist & writhe of kink-unstable magnetic flux ropes I flux rope: helicity sum of twist and writhe: kink instability: twist  and writhe  (sum is constant)
Three Dimensional Visualization of the Solar Corona and study of coronal cavity observed by Yohkoh/SXT and Hinode/XRT J. Okumura, D. Mineyama, H. Watanabe,
1Yang Liu/Magnetic FieldHMI Science – 1 May 2003 Magnetic Field Goals – magnetic field & eruptive events Yang Liu Stanford University.
AGU Dec 2000 The Structure and Evolution of a Sigmoid Observed During Whole Sun Month 3 Lyndsay Fletcher Sarah Gibson, and the WSM3 sigmoid structure working.
Observational Evidence for Magnetic Reconnection in the Solar Corona Len Culhane Mullard Space Science Laboratory University College London.
Observations of Eruptive Events with Two Radioheliographs, SSRT and NoRH V.V. Grechnev, A.M. Uralov, V.G. Zandanov, N.Y. Baranov, S.V. Lesovoi Kiyosato,
Helicity Condensation: The Origin of Coronal/Heliospheric Structure S. K. Antiochos, C. R. DeVore, et al NASA/GSFC Key features of the corona and wind.
Flare Energy Build-Up in a Decaying Active Region Near a Coronal Hole Yingna Su Smithsonian Astrophysical Observatory Collaborators: A. A. van Ballegooijen,
Measurement of the Reconnection Rate in Solar Flares H. Isobe 2004/12/6 Taiyo-Zasshikai.
NoRH Observations of Prominence Eruption Masumi Shimojo Nobeyama Solar Radio Observatory NAOJ/NINS 2004/10/28 Nobeyama Symposium SeiSenRyo.
Pre-flare activity of M1.2 flare 김수진 1,2, 문용재 1, 김연한 1, 박영득 1, 김갑성 2 1. Korea Astronomy and Space Science Institute 2. Kyung Hee University.
1 Introduction: Onset of solar flares and coronal mass ejections Yokoyama, T. Dept. Earth & Planetary Science, University of Tokyo Isobe, H. Univ. Tokyo.
ASAI Ayumi Kwasan Observatory, Kyoto University July 12, Evolution of Flare Ribbons and Energy Release.
Solar seminor: 4 Oct (1)Eruption of a multiple-turn helical magnetic flux tube in a large flare : Evidence for external and i ternal reconnection.
III. APPLICATIONS of RECONNECTION Yohkoh Bright Pts Loops Holes A magnetic world T=few MK 1. Coronal Heating.
SHINE Formation and Eruption of Filament Flux Ropes A. A. van Ballegooijen 1 & D. H. Mackay 2 1 Smithsonian Astrophysical Observatory, Cambridge,
Evolutionary Characteristics of Magnetic Helicity Injection in Active Regions Hyewon Jeong and Jongchul Chae Seoul National University, Korea 2. Data and.
X Visit For 100’s of free powerpoints.
What we can learn from active region flux emergence David Alexander Rice University Collaborators: Lirong Tian (Rice) Yuhong Fan (HAO)
Helicity Thinkshop 2009, Beijing Asymmetry of helicity injection in emerging active regions L. Tian, D. Alexander Rice University, USA Y. Liu Yunnan Astronomical.
Thought in 2000: Magnetic helicity is an important theoretical concept
Phillip Chamberlin Solar Flares (303) University of Colorado
TRACE Downflows and Energy Release
Abstract We simulate the twisting of an initially potential coronal flux tube by photospheric vortex motions. The flux tube starts to evolve slowly(quasi-statically)
Quantifying Reconnection*
Preflare State Rust et al. (1994) 太陽雑誌会.
Correlation between halo coronal mass ejections
Ron Moore and Alphonse Sterling
-Short Talk- The soft X-ray characteristics of solar flares, both with and without associated CMEs Kay H.R.M., Harra L.K., Matthews S.A., Culhane J.L.,
Downflow as a Reconnection Outflow
Magnetic Helicity In Emerging Active Regions: A Statistical Study
Filament/Prominence Eruption Corona Mass Ejection (CME)
Presentation transcript:

Observation of Sigmoids with Solar-B K.Hori (Hiraiso Solar Observatory, CRL)

Sigmoids Classification After Pevtsov 2002 Interlocking Loops (Eruptive) Multiple Loops Single Loop (Eruptive) Inter-Region Sigmoid

Secrets of Sigmoids   - Magnetic topology (e.g., helicity, shear buildup) Priest 1992; Titov et al.1993; Rust&Kumar 1996; Demoulin et al. 1997; Amari et al. 2000…. - Connection with Eruptions (e.g., missing mass deduced from dimming, CMEs) Hudson&Webb 1997; Sterling&Hudson 1997 Canfield et al. 2000; Glover et al. 2000….  - Formation and Evolution of Sigmoids Sigmoid→Arcade/Cusp Physical process involved in the formation of sigmoids is still not clear.

Formation of Sigmoids By linkage of two initially unconnected bipoles/ARs? Martens & Zwaan 2001 Formation of Sigmoids By emerging below the photosphere as a part of a twisted flux tube? Matsumoto et al. 1998; Magara and Longcope 2001,…  

Temperature Diagnosis of Interlocking Sigmoids 18-Oct-1994

Case1: AR Sigmoid 19-Oct-1994 Goes M3 SXT Al1+AlMg Moore et al. 2001  SXT Al1+AlMg 19:00:20-19:34:10 20:32:12-20:49:36 20:50:08-20:53:28 Flare Early in the rise phase (MK)

van Driel-Gesztelyi et al. 2000 Case2: AR Sigmoid 25-Oct-1994, C4.7 Manoharan et al.1996 van Driel-Gesztelyi et al. 2000  SXT Al1+AlMg 09:47:09-09:50:21 10:00:39-10:03:55 11:28:55-11:32:11 Short Loops (MK)

Case3: Sigmoidal Filament 8-May-2000 B6.8 Yohkoh SXT Hα 17GHz (NoRH) May 7 Hiraiso 10 km 5 May 8 Hida, FMT 04:35 04:00 04:26

17GHz dark patch: Manifestation of low temperature regions (Tb < 10 K ) 4 May 7 May 8 04:26:25 05:09:05 Heating has started. The midpoint remained to be cold.

Sigmoid Evolution in Hα 04:58:00 05:10:00 05:36:00 Bifurcation and disappearance of the eastern half of the filament. B6.8 Two-ribbon flare 08:09:31 SXT

Interlocking Sigmoids Magnetic Structure of Interlocking Sigmoids = + ? ?

Yohkoh SXT was the best observational tool to reveal the secrets of Sigmoids if..... the observations were not interrupted so often by Yohkoh nights. the SXR brightness of flare regions were not saturated. → Exposure time, temperature range velocity and magnetic field maps could be obtained simultaneously with temperature and EM maps. →XRT,SOT,EIS