Deconvolution of directly precipitating and trap-precipitating electrons in solar flare hard X-rays.: III.: Yohkoh hard X-Ray Telescope data analysis

被引:56
作者
Aschwanden, MJ
Fletcher, L
Sakao, T
Kosugi, T
Hudson, H
机构
[1] Lockheed Martin ATC, Solar & Astrophys Lab, Dept L941, Palo Alto, CA 94304 USA
[2] Natl Astron Observ, Tokyo 1818588, Japan
[3] Inst Space & Astronaut Sci, Kanagawa 2298510, Japan
[4] Solar Phys Res Corp, Tucson, AZ 85718 USA
关键词
acceleration of particles; radiation mechanisms : nonthermal; Sun : corona; Sun : flares; Sun; X-rays; gamma rays;
D O I
10.1086/307230
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We analyze the footpoint separation d and flux asymmetry A of magnetically conjugate double footpoint sources in hard X-ray images from the Yohkoh Hard X-Ray Telescope (HXT). The data set of 54 solar flares includes all events simultaneously observed with the Compton Gamma Ray Observatory (CGRO) in high time resolution mode. From the CGRO data we deconvolved the direct-precipitation and trap-precipitation components previously (in Paper II). Using the combined measurements from CGRO and HXT, we develop an asymmetric trap model that allows us to quantify the relative fractions of four different electron components, i.e., the ratios of direct-precipitating (q(P1), q(P2)) and trap-precipitating electrons (q(T1), q(T2)) at both magnetically conjugate footpoints. We find mean ratios of q(P1) = 0.14 +/- 0.06, q(P2) = 0.26 +/- 0.10, and q(T) = q(T1) + q(T2) = 0.60 +/- 0.13. We assume an isotropic pitch-angle distribution at the acceleration site and double-sided trap precipitation (q(T2)/q(T1) = q(P2)/q(P1)) to determine the conjugate loss-cone angles (alpha(1) = 42 degrees +/- 11 degrees and alpha(2) = 52 degrees +/- 10 degrees) and magnetic mirror ratios at both footpoints (R(1) = 1.6, ..., 4.0 and R(2) = 1.3, ..., 2.5). From the relative displacement of footpoint sources we also measure altitude differences of hard X-ray emission at different energies, which are found to decrease systematically with higher energies, with a statistical height difference of h(Lo) - h(M1) = 980 +/- 250 km and h(M1) - h(M2) = 310 +/- 300 km between the three lower HXT energy channels (Lo, M1, M2).
引用
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页码:977 / 989
页数:13
相关论文
共 27 条
[1]  
[Anonymous], 1986, NUMERICAL RECIPES C
[2]   Deconvolution of directly precipitating and trap-precipitating electrons in solar flare hard X-rays. I. Method and tests [J].
Aschwanden, MJ .
ASTROPHYSICAL JOURNAL, 1998, 502 (01) :455-467
[3]   Electron time-of-flight measurements during the Masuda flare, 1992 January 13 [J].
Aschwanden, MJ ;
Hudson, H ;
Kosugi, T ;
Schwartz, RA .
ASTROPHYSICAL JOURNAL, 1996, 464 (02) :985-998
[4]   The scaling law between electron time-of-flight distances and loop lengths in solar flares [J].
Aschwanden, MJ ;
Kosugi, T ;
Hudson, HS ;
Wills, MJ ;
Schwartz, RA .
ASTROPHYSICAL JOURNAL, 1996, 470 (02) :1198-1217
[5]   Electron time-of-flight distances and flare loop geometries compared from CGRO and Yohkoh observations [J].
Aschwanden, MJ ;
Wills, MJ ;
Hudson, HS ;
Kosugi, T ;
Schwartz, RA .
ASTROPHYSICAL JOURNAL, 1996, 468 (01) :398-417
[6]   Deconvolution of directly precipitating and trap-precipitating electrons in solar flare hard X-rays.: II.: Compton Gamma Ray Observatory data analysis [J].
Aschwanden, MJ ;
Schwartz, RA ;
Dennis, BR .
ASTROPHYSICAL JOURNAL, 1998, 502 (01) :468-480
[7]  
ASCHWANDEN MJ, 1999, IN PRESS APJ
[8]  
BASTIAN TS, 1999, UNPUB
[9]  
BASTIAN TS, 1988, ARA A, V36, P131
[10]   DIRECTIVITY AND POLARIZATION OF THICK TARGET X-RAY BREMSSTRAHLUNG FROM SOLAR-FLARES [J].
BROWN, JC .
SOLAR PHYSICS, 1972, 26 (02) :441-459