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相对论性电子-正电子对等离子体中磁重联的热惯性效应。

Thermal-inertial effects on magnetic reconnection in relativistic pair plasmas.

作者信息

Comisso Luca, Asenjo Felipe A

机构信息

Dipartimento Energia, Politecnico di Torino, Corso Duca degli Abruzzi 24, 10129 Torino, Italy and Istituto dei Sistemi Complessi-CNR, Via dei Taurini 19, 00185 Roma, Italy.

Facultad de Ingeniería y Ciencias, Universidad Adolfo Ibáñez, Santiago 7941169, Chile and Departamento de Ciencias, Facultad de Artes Liberales, Universidad Adolfo Ibáñez, Santiago 7941169, Chile.

出版信息

Phys Rev Lett. 2014 Jul 25;113(4):045001. doi: 10.1103/PhysRevLett.113.045001. Epub 2014 Jul 23.

Abstract

The magnetic reconnection process is studied in relativistic pair plasmas when the thermal and inertial properties of the magnetohydrodynamical fluid are included. We find that in both Sweet-Parker and Petschek relativistic scenarios there is an increase of the reconnection rate owing to the thermal-inertial effects, both satisfying causality. To characterize the new effects we define a thermal-inertial number which is independent of the relativistic Lundquist number, implying that reconnection can be achieved even for vanishing resistivity as a result of only thermal-inertial effects. The current model has fundamental importance for relativistic collisionless reconnection, as it constitutes the simplest way to get reconnection rates faster than those accessible with the sole resistivity.

摘要

当考虑磁流体动力学流体的热性质和惯性性质时,在相对论性电子-正电子等离子体中研究了磁重联过程。我们发现,在斯威特-帕克和佩切克相对论性情形中,由于热惯性效应,重联率都会增加,且二者都满足因果律。为了表征这些新效应,我们定义了一个热惯性数,它与相对论性伦德奎斯特数无关,这意味着仅由于热惯性效应,即使电阻率为零也能实现重联。当前模型对于相对论性无碰撞重联具有根本重要性,因为它构成了获得比重联率仅由电阻率决定时更快的重联率的最简单方法。

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