scholarly journals Solar flare hard X-ray spectra possibly inconsistent with the collisional thick target model

2006 ◽  
Vol 38 (5) ◽  
pp. 945-950 ◽  
Author(s):  
Eduard P. Kontar ◽  
John C. Brown
Keyword(s):  
X Ray ◽  
1990 ◽  
Vol 142 ◽  
pp. 445-447
Author(s):  
R. R. Rausaria ◽  
Ranjana Bakaya ◽  
P.N. Khosa

Solar flare hard X-ray data obtained by Prognoz-9 spacecraft (Abrosimov et al 1988) in the energy range 10-200 keV are analysed. In examples of events which we consider here, high energy X-ray pulses appear earlier than low energy ones, which is contrary to many other events where the low energy X-ray peak emission takes place earlier. The variation of the spectral index was dynamical.


Solar Physics ◽  
1983 ◽  
Vol 88 (1-2) ◽  
Author(s):  
J.C. Brown ◽  
V.A. Carlaw ◽  
D. Cromwell ◽  
S.R. Kane
Keyword(s):  
X Ray ◽  

2016 ◽  
Vol 818 (1) ◽  
pp. 44 ◽  
Author(s):  
J. W. Reep ◽  
S. J. Bradshaw ◽  
G. D. Holman

2009 ◽  
Vol 508 (2) ◽  
pp. 993-1000 ◽  
Author(s):  
J. C. Brown ◽  
R. Turkmani ◽  
E. P. Kontar ◽  
A. L. MacKinnon ◽  
L. Vlahos

1975 ◽  
Vol 68 ◽  
pp. 237-238
Author(s):  
Joan Vorpahl ◽  
Tatsuo Takakura

SummaryA study was made of the hard X-ray component in the impulsive phase of solar flares. In 36 randomly chosen events the value for the slope in the differential electron power spectrum E−δ electrons cm−2 s−1 keV−1, was related to the 20–32 keV spike rise time (e-folding) as trise = 0.56 exp (0.88δ) in the thin target model and tfrise = 0.10 exp (0.88δ) in the thick target picture. In the thin target model, the above empirical relation would imply that the acceleration of electrons can be longer when the acceleration rate is smaller. An alternative interpretation would be that an impulsive hard X-ray burst is a superposition of two components emitted from thin and thick targets; when the former predominates, the duration is longer and the photon spectral index is larger, while when the latter predominates, the duration is shorter and the photon spectral index is smaller; 3 ≲δ ≲4 is required (Figure 1). The uncertainty in δ is 0.5 while that in the rise time is 1 s.


2009 ◽  
Vol 705 (2) ◽  
pp. 1584-1593 ◽  
Author(s):  
Yang Su ◽  
Gordon D. Holman ◽  
Brian R. Dennis ◽  
Anne K. Tolbert ◽  
Richard A. Schwartz
Keyword(s):  

Solar Physics ◽  
1978 ◽  
Vol 58 (1) ◽  
pp. 139-148 ◽  
Author(s):  
Peter Hoyng ◽  
Joshua W. Knight ◽  
Daniel S. Spicer
Keyword(s):  

Space Weather ◽  
2015 ◽  
Vol 13 (5) ◽  
pp. 286-297 ◽  
Author(s):  
L. M. Winter ◽  
K. Balasubramaniam

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