INJECTION OF κ-LIKE SUPRATHERMAL PARTICLES INTO DIFFUSIVE SHOCK ACCELERATION

被引:28
|
作者
Kang, Hyesung [1 ]
Petrosian, Vahe [2 ,3 ,4 ]
Ryu, Dongsu [5 ]
Jones, T. W. [6 ]
机构
[1] Pusan Natl Univ, Dept Earth Sci, Pusan 609735, South Korea
[2] Stanford Univ, Dept Phys, Stanford, CA 94305 USA
[3] Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
[4] Stanford Univ, KIPAC, Stanford, CA 94305 USA
[5] UNIST, Dept Phys, Ulsan 689798, South Korea
[6] Univ Minnesota, Sch Phys & Astron, Minneapolis, MN 55455 USA
来源
ASTROPHYSICAL JOURNAL | 2014年 / 788卷 / 02期
基金
新加坡国家研究基金会; 美国国家科学基金会;
关键词
acceleration of particles; cosmic rays; shock waves; LOW-ENERGY ELECTRONS; STOCHASTIC ACCELERATION; THERMAL PROTONS; WAVES; DISTRIBUTIONS; SIMULATION; CLUSTERS;
D O I
10.1088/0004-637X/788/2/142
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We consider a phenomenological model for the thermal leakage injection in the diffusive shock acceleration (DSA) process, in which suprathermal protons and electrons near the shock transition zone are assumed to have the so called kappa-distributions produced by interactions of background thermal particles with pre-existing and/or self-excited plasma/MHD waves or turbulence. The kappa-distribution has a power-law tail, instead of an exponential cutoff, well above the thermal peak momentum. So there are a larger number of potential seed particles with momentum, above that required for participation in the DSA process. As a result, the injection fraction for the kappa-distribution depends on the shock Mach number much less severely compared to that for the Maxwellian distribution. Thus, the existence of kappa-like suprathermal tails at shocks would ease the problem of extremely low injection fractions, especially for electrons and especially at weak shocks such as those found in the intracluster medium. We suggest that the injection fraction for protons ranges 10(-4)-10(-3) for a kappa-distribution with 10 less than or similar to kappa(p) less than or similar to 30 at quasi-parallel shocks, while the injection fraction for electrons becomes 10(-6)-10(-5) for a kappa-distribution with kappa(e) less than or similar to 2 at quasi-perpendicular shocks. For such kappa values the ratio of cosmic ray (CR) electrons to protons naturally becomes K-e/p similar to 10(-3)-10(-2), which is required to explain the observed ratio for Galactic CRs.
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页数:8
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