相对论条纹风中激波驱动重联的粒子室模拟

L. Sironi, A. Spitkovsky
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引用次数: 18

摘要

通过二维和三维的粒子池模拟,研究了相对论条纹流终止激波下驱动磁重联的过程。在脉冲星风和磁驱动的相对论性喷流中,气流由交替磁场极性的条纹组成,由热等离子体的电流片隔开。在风终止激波处,流体被压缩,交变磁场被驱动磁重联湮灭。与条纹波长无关?或者风的磁化?(在政权????1(磁主导流),激波驱动的重联将交变场的所有磁能转移到粒子上,粒子的平均洛伦兹系数增加了?相对于冲击前值。在极限?/(rL?)??1,其中rL为风中的相对论拉莫尔半径,激波后粒子谱接近斜率约为?1.5的平坦幂律尾巴,由重联电场加速的粒子填充。电流导向的存在?只有当引导场大于交变分量时,磁场才能抑制粒子的加速度。我们的发现对脉冲星风星云和相对论喷流的非热辐射模型提出了重要的限制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Particle-in-cell simulations of shock-driven reconnection in relativistic striped winds
By means of two- and three-dimensional particle-in-cell simulations, we investigate the process of driven magnetic reconnection at the termination shock of relativistic striped flows. In pulsar winds and in magnetar-powered relativistic jets, the flow consists of stripes of alternating magnetic field polarity, separated by current sheets of hot plasma. At the wind termination shock, the flow compresses and the alternating fields annihilate by driven magnetic reconnection. Irrespective of the stripe wavelength ? or the wind magnetization ? (in the regime ????1 of magnetically dominated flows), shock-driven reconnection transfers all the magnetic energy of alternating fields to the particles, whose average Lorentz factor increases by a factor of ? with respect to the pre-shock value. In the limit ?/(rL?)???1, where rL is the relativistic Larmor radius in the wind, the post-shock particle spectrum approaches a flat power-law tail with slope around ?1.5, populated by particles accelerated by the reconnection electric field. The presence of a current-aligned ?guide? magnetic field suppresses the acceleration of particles only when the guide field is stronger than the alternating component. Our findings place important constraints on the models of non-thermal radiation from Pulsar Wind Nebulae and relativistic jets.
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