Diffusion in pulsar wind nebulae: an investigation using magnetohydrodynamic and particle transport models

被引:66
|
作者
Porth, O. [1 ,2 ]
Vorster, M. J. [3 ,4 ]
Lyutikov, M. [3 ]
Engelbrecht, N. E. [4 ]
机构
[1] Inst Theoret Phys, D-60438 Frankfurt, Germany
[2] Univ Leeds, Dept Appl Math, Leeds LS2 9JT, W Yorkshire, England
[3] Purdue Univ, Dept Phys, 525 Northwestern Ave, W Lafayette, IN 47907 USA
[4] North West Univ, Ctr Space Res, ZA-2520 Potchefstroom, South Africa
基金
美国国家科学基金会;
关键词
diffusion; MHD; turbulence; pulsars: individual: 3C 58; pulsars: individual: G21.5-09; pulsars: individual: Vela; X-RAY OBSERVATIONS; CRAB-NEBULA; PSR J1833-1034; MAGNETIC-FIELD; YOUNG PULSAR; PERPENDICULAR DIFFUSION; NONTHERMAL EMISSION; VELA PULSAR; INNER KNOT; SIMULATIONS;
D O I
10.1093/mnras/stw1152
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We study the transport of high-energy particles in pulsar wind nebulae (PWN) using three-dimensional magnetohydrodynamic (MHD) and test-particle simulations, as well as a Fokker-Planck particle transport model. The latter includes radiative and adiabatic losses, diffusion, and advection on the background flow of the simulated MHD nebula. By combining the models, the spatial evolution of flux and photon index of the X-ray synchrotron emission is modelled for the three nebulae G21.5-0.9, the inner regions of Vela, and 3C 58, thereby allowing us to derive governing parameters: the magnetic field strength, average flow velocity, and spatial diffusion coefficient. For comparison, the nebulae are also modelled with the semi-analytic Kennel & Coroniti model but the Porth et al. model generally yields better fits to the observational data. We find that high velocity fluctuations in the turbulent nebula (downstream of the termination shock) give rise to efficient diffusive transport of particles, with average P,clet number close to unity, indicating that both advection and diffusion play an important role in particle transport. We find that the diffusive transport coefficient of the order of similar to 2 x 10(27)(L-s/0.42 Ly) cm(2) s(- 1) (L-s is the size of the termination shock) is independent of energy up to extreme particle Lorentz factors of gamma(p) similar to 10(10).
引用
收藏
页码:4135 / 4149
页数:15
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