POLARIZED SYNCHROTRON EMISSIVITIES AND ABSORPTIVITIES FOR RELATIVISTIC THERMAL, POWER-LAW, AND KAPPA DISTRIBUTION FUNCTIONS

被引:63
作者
Pandya, Alex [1 ]
Zhang, Zhaowei [1 ]
Chandra, Mani [2 ]
Gammie, Charles F. [1 ,2 ]
机构
[1] Univ Illinois, Dept Phys, 1110 W Green St, Urbana, IL 61801 USA
[2] Univ Illinois, Dept Astron, 1002 W Green St, Urbana, IL 61801 USA
基金
美国国家科学基金会;
关键词
plasmas; polarization; radiation mechanisms: general; radiative transfer; relativistic processes; SGR A-ASTERISK; RADIATION; EMISSION; PLASMAS; CYCLOTRON; ELECTRONS;
D O I
10.3847/0004-637X/822/1/34
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Synchrotron emission and absorption determine the observational appearances of many astronomical systems. In this paper, we describe a numerical scheme for calculating synchrotron emissivities and absorptivities in all four Stokes parameters for arbitrary gyrotropic electron distribution functions, building on earlier work by Leung, Gammie, and Noble. We use this technique to evaluate the emissivities and the absorptivities for a thermal (Maxwell-Jutttner), isotropic power-law, and an isotropic kappa distribution function. The latter contains a power-law tail at high particle energies that smoothly merges with a thermal core at low energies, as is characteristic of observed particle spectra in collisionless plasmas. We provide fitting formulae and error bounds on the fitting formulae for use in codes that solve the radiative transfer equation. The numerical method and the fitting formulae are implemented in a compact C library called symphony. We find that the kappa distribution has a source function that is indistinguishable from a thermal spectrum at low frequency and transitions to the characteristic self-absorbed synchrotron spectrum, proportional to nu(5/2) 2, at high frequency; the linear polarization fraction for a thermal spectrum is near unity at high frequency; and all distributions produce O(10%) circular polarization at low frequency for lines of sight sufficiently close to the magnetic field vector.
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页数:10
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