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Published byClarence McDonald Modified over 9 years ago
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Joint session WG4/5 Points for discussion: - Soft-hard-soft spectral behaviour – again - Non-thermal pre-impulsive coronal sources - Very dense coronal loops (~ 10 11 cm -3 ) and other dense structures - Coronal sources that decrease in altitude (sometimes as footpoints approach), then increase - tiny inferred size of flare footpoints high beam flux and implications
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30-50 keV intensity 30-50 keV / 20-30 keV intensity ratio 50-70 keV / 30-50 keV intensity ratio Correlation between impulsive phase intensity and spectral hardness - ubiquitous Spectral soft – hard - soft
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GOES 1-8 A DERIVATIVE Non-thermal preflare coronal sources
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RHESSI Preflare Maps 3-12 keV (color): 12-25 keV (contours) 01:07:00-01:08:30 01:08:00-01:10:30 01:11:00-01:12:30 Coronal source
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RHESSI SPECTRA 5-50 keV Thermal+broken powerlaw Preflare period: 01:02:00-01:11:00 Broken powerlaw extends down to 5 keV Thermal component never dominates EM and T are poorly determined Chisquare ~ 1 if EM=0 White = photons, Green = thermal model, Red = broken powerlaw, Purple = background (NB similar source in July 23 rd 2002 event)
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Dense coronal sources Substantial high energy emission in corona: thermal and radio observations allow estimate of density – 10 11 cm -3 20-30 keV30-50 keV50-100 keV 20 July 2002, pixon image reconstruction
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Descending loop top sources Time evolution: blue white Footpoints: 70-100 keV Loop top: 20-25 keV
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H footpoint separation HXR source ‘height’ Descending loop top sources – with decreasing footpoint separation
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Flare footpoints – white light observations WL coincides with HXR source locations – sizes at resolution of TRACE (few px = few 1000 km area ~ 10 17 cm 2 )
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M2.2 flare Predicted ‘evaporation’ velocity as function of beam flux Using A= 10 18 cm 2 Using A= 10 17 cm 2
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