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Solar-B Science Objectives - Overview of the Mission -. Kazunari Shibata (Kyoto Univ.). Science Objectives of Solar-B Mission. Kosugi (1999) coronal heating coronal dynamics and structure elementary processes such as reconnection. chromospheric heating, spicules, ….
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Solar-B Science Objectives- Overview of the Mission - Kazunari Shibata (Kyoto Univ.)
Science Objectives of Solar-B Mission Kosugi (1999) • coronal heating • coronal dynamics and structure • elementary processes such as reconnection chromospheric heating, spicules, … jets, prominence, CME, solar wind, waves/shocks,… reconnection jet, inflow, slow/fast shocks,… - emerging flux and dynamo flux tubes, sunspots, convection, …
These Objectives are also important for astrophysics and space weather • To explore solar MHD as a laboratory of astrophysical MHD • To explore solar activity as a basis of space weather research
Plan of this talk • Introduction – Main Instruments • Main Objectives • Coronal and Chromospheric Heating Nanoflares, Alfven Waves, Spicules • Coronal Dynamics and Structure Jets, CMEs, Coronal Waves/Shocks • Reconnection • Emerging Flux • Summary
Solar-B Mission • Solar Optical Telescope (SOT) • X-Ray Telescope (XRT) • EUV Imaging Spectrometer (EIS) • Launch Date: 2005 J-fiscal year • Mission Lifetime: > 3 years • Orbit: Polar, Sun Synchronous
Solar Optical Telescope (SOT) • 50 cm Aplanatic Gregorian – Japan • Focal Plane Package – US(LMATC) (Filtergram+Spectro-polarimeter) • => 0.2 arsec resolution; 380-700 km vector magnetic field measurements
X-Ray Telescope (XRT) • Grazing-Incidence Optics – US(SAO) • CCD Camera – Japan • => 1 arcsec resolution; 1 – 30 MK
EUV Imaging Spectrometer (EIS) • 15 cm Offset Parabolic Mirror, Slit/Slot & Multilayer Grating – US (NRL, GSFC) • Camera – UK(MSSL,RAL,Birmingham) • Controller – Japan • 20 km/s nonthermal motion • 2 arcsec spatial resolution • Temperature coverage 0.1 – 20 MK
太陽活動の11年周期 黒点数
Yohkoh HXT Flares in 1991-1998 2005 - 2007
2005 Nov Predicted Solar Corona in 2005-2007 2007Sep(minimum) • Sep (minimum) • 2007 Sep ? 1994 Nov 2005 Nov ?
Coronal HeatingAlfven wave vs Nanoflare • Alfven Wave heating • Nanoflare heating
Nanoflare Heating ? • Shimizu (1995) Ph. D. Thesis active region corona is filled withmicroflare/nanoflare => nanoflare heating ? • Kano (1997) Ph. D. Thesis loop top heating ? • Priest et al. (1998) nanoflare heating ?
Microflare/Nanoflare Occurrence Frequency α=1.6-1.7 <2 Shimizu, Shimojo, Aschwanden, …. => insufficient for coronal heating α>2 Krucker & Benz
Alfven Wave Heating ? • Yashiro (2000) Ph. D. Thesis Lx(active region) ∝ B^1.07 F ∝ B => Alfven wave heating ?
Alfven wave theory of Spiculesand Coronal Heating(Hollweg et al. 1982, Kudoh-Shibata 1999) Hα (Hida DST)
Alfven wave model of spicules:numerical simulation (Kudoh-Shibata 1999)
Energy Flux Carried by Alfven Waves into Corona (Saitoh, Kudoh, Shibata 2001)
Question on Coronal Heating • What is the true occurrence frequency of nanoflare ? • What is the heating rate and its dependence upon magnetic field ? • What is the energy flux carried by Alfven waves into the corona ? • What is the origin of Alfven waves ? Photospheric turbulence or reconnection ?
Coronal Dynamics and Structure: X-ray Jet Yokoyama & Shibata (1995)
CDS spinning jet (Pike&Mason) Zoo of Solar Jets • H alpha jets (surges) • EUV macrospicules • EIT jets • LASCO jets Cosmic jet (HST) H alpha spinning jet (Kurokawa) EIT-LASCO jet (Wang, Y. M.)
Polar plume Evaporation flow produced by reconnection heating ? (Wang, Y.M. 1999)
Moreton Wave(Hα:Hida FMT, Eto et al. 2001) Moreton wave = Fast mode MHD shock (Uchida 1968)
Wave front of Moreton wave Propagation speed ~ 720km/s 5:55
5:40 - 5:31 5:58 - 5:40 ② ① 6:14 - 5:58 6:31 - 6:14 ③ ④
Moreton wave and EIT wave EIT wave EIT wave (Thompson et al. 1998) Moreton wave
Question on Coronal Dynamics and Structure (Jets and Waves) • What is the true velocity of X-ray jets ? • What is the acceleration mechanism of X-ray jets ? ( => Shimojo’s talk) • What is the relation to coronal heating and acceleration of high speed solar wind ? • What is EIT wave ? • What is the origin of Moreton wave ?
Reconnection • Yohkoh found plenty of evidence of reconnection in flares. • But we have not seen reconnection jet and inflow in SXT images. (but see Yokoyama et al. 2000 ApJ Let.)
Reconnection Rate of a Cusp-Shaped Flare on May 12, 1997(Isobe et al. => poster) Reconnection rate is high even in a very late decay phase V_inflow/V_A= 0.001 – 0.01
Question on Reconnection • Are there really high speed reconnection jets with 1000 km/s ? • What is the reconnection rate (inflow speed) in solar flares, jets, and coronal mass ejections ? • What determines the reconnection rate ? => Yokoyama’s talk
Emerging Flux Region Emerging Flux Region (EFR) is important for (1) Dynamic Phenomena (2) Dynamo (3) Coronal Heating
TRACE Observation of Emerging Flux Wavelength ~ 171 A Time cadence~ 1 min Spatial Resolution ~ 2 arcsec Dark : Chromosphere Bright : Corona
Comparison with SXT (Yashiro-Shibata) TRACE SXT
Emergence of twisted flux tube - most fundamental driver of solar activity ? - (Matsumoto et al. 1998)
Question on Emerging Flux • How and when are kG intense flux tubes created in emerging flux ? • How and why are twisted emeging flux tubes generated ? • Will we observe flare-like explosive reconnection (with jets and shocks) in photospheric reconnection associated with emerging flux ?
Summary • More, smaller, and fasterjets, plasmoids, waves, and shocks would be found by Solar-B. • High time cadence velocity field observations (with EIS and SOT) with good coordination with XRT is extremely important.