结构化固体靶上入射的极强激光脉冲产生 $e^-e^+$ 等离子体并使其磁性自约束

Alexander Samsonov, Alexander Pukhov
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引用次数: 0

摘要

我们提出了一种用于产生高密度、相对论性、强磁化电子-正电子对等离子体的全光学、单激光脉冲方案。该方案涉及极强($I \gtrsim\SI{e24}{watt/\cm^2}$)圆偏振激光脉冲与包含锥形腔的固体密度目标的相互作用。通过考虑量子电动力学效应的全尺度三维腔内粒子(Particle-in-cell,PIC)模拟,结果表明这种相互作用产生了两个重要结果:第一,由于反法拉第效应产生了高达数十千兆高斯的准静态轴向磁场;第二,通过布赖特-维勒过程产生了大量电子-正电子对(高达 $\num{e13}$)。e^-e^+$等离子体会被困在磁场中,并保持数百飞秒,远远超过激光的时间尺度。我们讨论了对等离子体参数的依赖性,以及等离子体产生和禁锢的效率与激光脉冲和目标特性的关系。通过实验实现这一方案将能够研究与极端天体物理环境相关的物理过程。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Production and magnetic self-confinement of $e^-e^+$ plasma by an extremely intense laser pulse incident on a structured solid target
We propose an all-optical, single-laser-pulse scheme for generating dense, relativistic, strongly-magnetized electron-positron pair plasma. The scheme involves the interaction of an extremely intense ($I \gtrsim \SI{e24}{\watt/\cm^2}$) circularly polarized laser pulse with a solid-density target containing a conical cavity. Through full-scale three-dimensional particle-in-cell (PIC) simulations that account for quantum electrodynamical effects, it is shown that this interaction results in two significant outcomes: first, the generation of quasi-static axial magnetic fields reaching tens of gigagauss due to the inverse Faraday effect; and second, the production of large quantities of electron-positron pairs (up to $\num{e13}$) via the Breit-Wheeler process. The $e^-e^+$ plasma becomes trapped in the magnetic field and remains confined for hundreds of femtoseconds, far exceeding the laser timescale. The dependency of pair plasma parameters, as well as the efficiency of plasma production and confinement, is discussed in relation to the properties of the laser pulse and the target. Realizing this scheme experimentally would enable the investigation of physical processes relevant to extreme astrophysical environments.
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