X-ray observations of Solar Flares. Marina Battaglia Fachhochschule Nordwestschweiz (FHNW)

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X-ray observations of Solar Flares Marina Battaglia Fachhochschule Nordwestschweiz (FHNW) marina.battaglia@fhnw.ch

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The solar corona Close by astrophysical laboratory allows us to study: Release of magnetic energy (magnetic reconnection) Particle acceleration Coronal heating Highly dynamic release of magnetic energy: Solar flares, coronal mass ejections (CMEs), solar wind Creates space weather 4

Solar flares open questions Where and how is magnetic energy released? Where and how are particles accelerated? How are particles transported? away from the Sun close to the Sun How much energy is contained in flares? How do flares affect all layers of the solar atmosphere? 5

The standard solar flare model 1) Release of magnetic energy Corona Chromosphere Shibata et al. 1995 Photosphere 6

The standard solar flare model 1) Release of magnetic energy Corona Google: Hudson Flare Cartoon http://solarmuri.ssl.berkeley.edu/~hhudson/cartoons/ Chromosphere Shibata et al. 1995 Photosphere 7

The standard solar flare model 1) Release of magnetic energy Corona Chromosphere Shibata et al. 1995 Photosphere 8

The standard solar flare model magnetic reconnection 1) Release of magnetic energy 2) Particle acceleration and heating e - Shibata et al. 1995 9

The standard solar flare model magnetic reconnection 1) Release of magnetic energy 2) Particle acceleration and heating 3) Accelerated electrons produce hard X-ray (HXR) emission and heat chromosphere e - Shibata et al. 1995 HXR footpoints 10

The standard solar flare model magnetic reconnection 1) Release of magnetic energy 2) Particle acceleration and heating 3) Accelerated electrons produce hard X-ray (HXR) emission and heat chromosphere 4) Chromospheric evaporation fills loop e - Shibata et al. 1995 HXR footpoints 11

The standard solar flare model magnetic reconnection HXR loop top source 1) Release of magnetic energy 2) Particle acceleration and heating 3) Accelerated electrons produce hard X-ray (HXR) emission and heat chromosphere 4) Chromospheric evaporation fills loop e - SXR Loop HXR footpoints HXR Footpoints Shibata et al. 1995 12

X-ray imaging spectroscopy EUV image Thermal bremsstrahlung: hot plasma in the flaring loop à temperature and emission measure of heated plasma à total thermal energy involved, flare driven heating, cooling Krucker & Battaglia 2014 Non-thermal bremsstrahlung from accelerated electrons à spectrum of accelerated electrons à total energy in accelerated electrons. acceleration mechanism 13

Solar flare observations with RHESSI The Reuven Ramaty High Energy Solar Spectroscopic Imager (RHESSI) Since 2002 9 Germanium detectors (7x7x8.5cm) ~3 kev 10 MeV energy resolution 1 kev @ 100 kev 3 kev @ 2223 kev spatial resolution 3 arcsec à Energy and time of incident photons Lin et al. 2002 14

Electron acceleration in above-the-looptop sources Low ambient density & strong X-ray source à very large number of accelerated electrons à Entire plasma is accelerated (non-thermal) in bulk energization process Masuda et al. 1994 pre-flare ambient f Above the loop-top-source is acceleration region flare accelerated v RHESSI imaging spectroscopy in combination with SDO/AIA observations à ambient density = accelerated electron density n nt ~10 9 cm -3 v Krucker et al. 2010 Krucker & Battaglia 2014 15

Acceleration and transport of electrons vs ions Location of 200 300 kev emission (signature of accelerated electrons) Hurford et al. 2006 and 2218 2228 kev emission (neutron capture line, signature of accelerated ions) are displaced (Hurford et al. 2003, Hurford et al. 2006)! Different acceleration of electrons and ions? Different transport effects? 16

Energy deposition and atmospheric response Chromospheric evaporation observed with RHESSI and IRIS IRIS: Dopplershifts of FeXXI (10 MK) line à location and speed of evaporating plasma RHESSI: location and power of electron beam deposited energy -87 km/s Fe XXI Si II Fe II H 2 Si II Fe II C I Fe II Fe II 17

The future of solar flare X-ray observations ESA s Solar Orbiter & the STIX instrument Launch October 2018 2.5 years cruise phase 3 years primary science phase Swiss involvement in 3 instruments 18

The Spectrometer/Telescope for Imaging X-rays (STIX) Tungsten grids Imager Set of Beryllium window tungsten Germany CH grids separated by 55 cm Detector Electronics Module Detector with 32 Electronics detectors Module CdTe detectors (Caliste SO) DEM Poland France Czech Republic CH X-ray windows and feed-through CH in heat shield 19! 19

Summary and conclusions Solar flares allow us to study fundamental and universal physical processes such as magnetic energy release, particle acceleration, and particle transport in magnetised plasmas X-ray observations of solar flares serve as diagnostic of flare accelerated particles and hot plasma Need simultaneous observations at many wavelengths for full understanding of solar flares Look forward to Solar Orbiter for new view of solar activity and space weather 20