IMAGING SPECTROSCOPY ON PREFLARE CORONAL NONTHERMAL SOURCES ASSOCIATED WITH THE 2002 JULY 23 FLARE

被引:11
作者
Asai, Ayumi [1 ]
Nakajima, Hiroshi [1 ]
Shimojo, Masumi [1 ]
Yokoyama, Takaaki [2 ]
Masuda, Satoshi [3 ]
Krucker, Saem [4 ]
机构
[1] Natl Inst Nat Sci, Natl Astron Observ Japan, Nobeyama Solar Radio Observ, Minamisa Ku, Minamimaki, Nagano 3841305, Japan
[2] Univ Tokyo, Dept Earth & Planetary Sci, Bunkyo Ku, Tokyo 1130033, Japan
[3] Nagoya Univ, Solar Terr Environm Lab, Chikusa Ku, Nagoya, Aichi 4648601, Japan
[4] Univ Calif Berkeley, Space Sci Lab, Berkeley, CA 94720 USA
关键词
acceleration of particles; Sun: corona; Sun: flares; Sun: radio radiation; Sun:; X-rays; gamma rays; HARD X-RAYS; SOLAR-FLARES; PARTICLE-ACCELERATION; TRANSITION REGION; ELECTRONS; EMISSION; MICROWAVES; EXPLORER; NOBEYAMA; BURSTS;
D O I
10.1088/0004-637X/695/2/1623
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a detailed examination on the coronal nonthermal emissions during the preflare phase of the X4.8 flare that occurred on 2002 July 23. The microwave (17 GHz and 34 GHz) data obtained with Nobeyama Radioheliograph, at Nobeyama Solar Radio Observatory and the hard X-ray (HXR) data taken with RHESSI obviously showed nonthermal sources that are located above the flare loops during the preflare phase. We performed imaging spectroscopic analyses on the nonthermal emission sources both in microwaves and in HXRs, and confirmed that electrons are accelerated from several tens of keV to more than 1 MeV even in this phase. If we assume the thin-target model for the HXR emission source, the derived electron spectral indices (similar to 4.7) is the same value as that from microwaves (similar to 4.7) within the observational uncertainties, which implies that the distribution of the accelerated electrons follows a single power law. The number density of the microwave-emitting electrons is, however, larger than that of the HXR-emitting electrons, unless we assume low-ambient plasma density of about 1.0 x 10(9) cm(-3) for the HXR-emitting region. If we adopt the thick-target model for the HXR emission source, on the other hand, the electron spectral index (similar to 6.7) is much different, while the gap of the number density of the accelerated electrons is somewhat reduced.
引用
收藏
页码:1623 / 1630
页数:8
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