The Sun Understanding our Star with Polarimetry Silvano Fineschi INAF – Astrophysical Observatory of Torino - Italy Internatonal School of Astropolarimetry.

Slides:



Advertisements
Similar presentations
Electro-optical Spectro-polarimeter for Ground- and Space-based
Advertisements

What is the fate of our sun and other stars?
High Altitude Observatory (HAO) – National Center for Atmospheric Research (NCAR) The National Center for Atmospheric Research is operated by the University.
Coronal Magnetograph for Space and Ground-based Solar Observatories Silvano Fineschi Alessandro Bemporad, Gerardo Capobianco, Jessica Girella INAF –Astrophysical.
COSPAR E July 22, Paris revised for Nobeyama Symposium 2004 October 29, Kiyosato Takeo Kosugi (ISAS/JAXA, Japan)
ILWS 12 June 2007 ASI Program Ester Antonucci. Participation In Flight Missions SOHO (UVCS)SOHO (UVCS) UlyssesUlysses CLUSTERCLUSTER DOUBLE STARDOUBLE.
Our Star, the Sun Chapter Eighteen.
Chapter 8 The Sun – Our Star.
High Altitude Observatory (HAO) – National Center for Atmospheric Research (NCAR) The National Center for Atmospheric Research is operated by the University.
High Altitude Observatory (HAO) – National Center for Atmospheric Research (NCAR) The National Center for Atmospheric Research is operated by the University.
The High Altitude Observatory (HAO) at the National Center for Atmospheric Research (NCAR) The National Center for Atmospheric Research is sponsored by.
High Altitude Observatory (HAO) – National Center for Atmospheric Research (NCAR) The National Center for Atmospheric Research is operated by the University.
General Properties Absolute visual magnitude M V = 4.83 Central temperature = 15 million 0 K X = 0.73, Y = 0.25, Z = 0.02 Initial abundances: Age: ~ 4.52.
“The Role of Atomic Physics in Spectroscopic Studies of the Extended Solar Corona” – John Kohl “High Accuracy Atomic Physics in Astronomy”, August.
High Altitude Observatory (HAO) – National Center for Atmospheric Research (NCAR) The National Center for Atmospheric Research is operated by the University.
1 Grades 3 - 5: Introduction. 2 Better Observation Of The Sun And Earth Importance of Space Technology.
Capabilities of UV Coronagraphic Spectroscopy for Studying the Source Regions of SEPs & the Solar Wind John Kohl, Steven Cranmer, Larry Gardner, Jun Lin,
Do magnetic waves heat the solar atmosphere? Dr. E.J. Zita The Evergreen State College Fri.30.May 2003 at Reed College NW Section.
Alfvén Waves in the Solar Corona S. Tomczyk, S. Mclntosh, S. Keil, P. Judge, T. Schad, D. Seeley, J. Edmondson Science, Vol. 317, Sep., 2007.
Nour-Eddine Raouafi Magnetic and Velocity Fields in the Solar Corona Outline Polar Holes: Latest Results SUMER: The Polarimeter Conclusions.
Coronal magnetic field observations Useful coronal field model constraints can be obtained from IR observations This is a vigorous activity, with three.
Physical Astronomy Professor Lee Carkner Lecture 11
1.B – Solar Dynamo 1.C – Global Circulation 1.D – Irradiance Sources 1.H – Far-side Imaging 1.F – Solar Subsurface Weather 1.E – Coronal Magnetic Field.
Spectroscopic Diagnostics of Solar Wind, CME, and SEP Source Regions Imaging Workshop, NSSTC, Huntsville, AL, 9-10 November 2004 Spectroscopic Diagnostics.
990901EIS_RR_Science.1 Science Investigation Goals and Instrument Requirements Dr. George A. Doschek EIS US Principal Investigator Naval Research Laboratory.
Physical analogies between solar chromosphere and earth’s ionosphere Hiroaki Isobe (Kyoto University) Acknowledgements: Y. Miyoshi, Y. Ogawa and participants.
Coronal Heating of an Active Region Observed by XRT on May 5, 2010 A Look at Quasi-static vs Alfven Wave Heating of Coronal Loops Amanda Persichetti Aad.
Note key, please leave in binder. Our Sun
The Sun a medium sized star 93,000,000 miles away 109 times diameter of Earth 1 million Earths could fit in the Sun Made of gas: 82% hydrogen, 17% helium,
The Sun and the Heliosphere: some basic concepts…
Solar local and global magnetism new challenge for long-lasting synoptic observations. (Topic 1. New and continuing scientific questions) A.Kučera, P.
By: Kiana and Meagan. Purpose  To measure solar magnetic fields  To understand how energy generated by magnetic-field changes in the lower solar atmosphere.
Atmospheric transport and chemistry lecture I.Introduction II.Fundamental concepts in atmospheric dynamics: Brewer-Dobson circulation and waves III.Radiative.
SHINE 2008, June 23-27, Utah Observational Test of Coronal Magnetic Field Models I. Comparison with Potential Field Model Hao-Sheng Lin & Yu Liu Institute.
Space Research Institute Graz Austrian Academy of Sciences CERN, Geneve, June 2006 Helmut O. Rucker Exploring the Planets and Moons in our Solar System.
Probing Coronal Magnetism with Multi-wavelength Polarimetry Silvano Fineschi INAF-Torino Astrophysical Observatory, Italy 25 May, 2013, Bern (CH)
Coronal Spectro- polarimetry with the Turin Lyot-Filter Silvano Fineschi INAF – Astrophysical Observatory of Torino, Italy Future of Polarimetry - Brussels.
_________________at the centre of our solar system.
The Sun.
Predicting Solar Energetic Particle Events John Davis, Ron Moore, Edward West, Allen Gary NASA/MSFC/NSSTC Solar and Space Physics and the Vision for Space.
1 THE SUN Nada Al-Haddad KU Leuven SHINE OUTLINES Properties Core Radiative Zone Convective Zone Photosphere Chromosphere Corona 2.
SUN, EARTH AND SPACE. THE SUN CLOSE UP: INSIDE AND OUT.
SOLAR FLARES AND ERUPTIONS Lyndsay Fletcher University of Glasgow.
The Sun The Sun imaged in white light by the SOHO spacecraft.
Mass loss and Alfvén waves in cool supergiant stars Aline A. Vidotto & Vera Jatenco-Pereira Universidade de São Paulo Instituto de Astronomia, Geofísica.
Chapter 9 Our Star, the Sun. What do you think? What is the surface of the Sun like? Does the Sun rotate? What makes the Sun shine?
“Ambipolar Diffusion” and Magnetic Reconnection Tsap Yu. T
Shock heating by Fast/Slow MHD waves along plasma loops
The Sun…a star in our solar system (continued). But first…see a solar twin tonight Beta Canum Venaticorum…look almost up and a little east at 9PM.
Our Star, the Sun. The Sun is the Largest Object in the Solar System The Sun contains more than 99.85% of the total mass of the solar system If you.
MASC: Magnetic Activity of the Solar Corona Frédéric Auchère, Jean-Claude Vial Institut d’Astrophysique Spatiale, France Weiqun Gan, Hui Li Purple Mountain.
OUR SUN.
Sun: General Properties
Solar atmosphere.
The Sun: Portrait of a G2V star
The Sun: close-up of a spectral class G main sequence star
What is the fate of our sun and other stars?
The Sun and the Moon.
How does the solar atmosphere connect to the inner heliosphere?
Overview of the Sun Jie Zhang Art Poland
The Sun Chapter 17.
Introduction to Space Weather
Vector polarimetry with HMI
Chapter 9 The Sun.
The Sun.
OUR SUN.
Grades 3 - 5: Introduction
The Centre of the Solar System Earth Science 11
Grades 3 - 5: Introduction
8-11 The Sun Astronomy November 18, 2008 Sanders.
Presentation transcript:

The Sun Understanding our Star with Polarimetry Silvano Fineschi INAF – Astrophysical Observatory of Torino - Italy Internatonal School of Astropolarimetry Centre Paul Langevin Aussois (F), 3-8 June 2013

The Solar Dynamo: Powering the Sun’s magnetic field In the Sun, the magnetic field generated by the dynamo mechanism plays a central role in the dynamics of the solar atmosphere. Solar polarity reverses in about 11 years (solar cycle) The plasma dynamics in the solar atmosphere goes from being dominated by thermal pressure (kT) over the magnetic pressure (B 2 ) in the photosphere (1  )

The Solar Magnetic Field: Powering the Sun’s atmosphere Magnetic reconnection powers solar flares and Coronal Mass Ejections Magnetic waves (Alfven, acoustic)/reconnection (nanoflares) (TBD) power the solar wind

Solar Filter-Magnetograph

Solar Spectro- Polarimeter

Hanle Effect (tutorial)  Larmour << A  Larmour  A

Hanle effect in photospheri c lines

Hanle effect in chromospheric HI Lyman-  line

CLASP sounding-rocket: measuring the Hanle effect in HI Lyman- 

A [10 7 s -1 ] ~ 0.88  g J  B [G] Hanle effect Sensitivity in coronal lines A FeXIII = 14 Hz  B Hanle   G A FeXIII << B corona (“saturated” Hanle effect) Fineschi, van Ballegooijen & Kohl, 1999

Hanle Effect (tutorial)  Larmour >> A If  Larmour >> A (VIR forbidden lines)  P is // or  B A FeXIII = 14 Hz  B Hanle   G A FeXIII << B corona (“saturated” Hanle effect)

22 HAO CoMP LC Lyot fiter & Polarimeter FeXIII nm «forbidden line» S. Tomczyk, et al. Science 317, 1192 (2007);

Resonance-scattering Polarization

Fineschi, ASP Conf. Series, 2001 Anisotropic Super-radial Doppler-dimming effect OVI nm Doppler-dimming; CII pumping (S. Giordano courtesy)

SUMER Measurement of Hanle and ASD effects? P=(9  2)%;  = 9  6  Helioctr. Dist. = 1.3 R Wind speed w  40 km/s (Rauoafi A&A 1999) Hanle effect: B > 10 G;  B 50 km/s SR Doppler-dim.: B 30  ; w > 50 km/s Anisotr. SR Doppler-dim.: B <<1 G;  B  20  ; w  40 km/s (Fineschi ASP Conf. Series 2001)

SolmeX – COMPASS (ESA M-mission) Peter, Fineschi et al. Exp. Astron. 2011

Coronal UV Spectro-Polarimeter (CUPS)

Moses, et al. SPIE 2011 Non-Formation Flying CUPS Telescope externally occulted with multi-stacked apertures

Beta 1.05 Ro 10 Ro 2 Ro Temp. minimum Probing Coronal Magnetism with Space EUV/UV/VIR Polarimetry Photospheric VIR lines CIV 150 nm MgII h & k 280 nm HI Lyman series, OVI nm & Fe IR lines HI Ly-  122 nm SUMI CLASP SolmeX