等离子体中强激光脉冲的传播与尾流场的产生

E. Esarey, P. Sprangle, J. Krall, G. Joyce
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引用次数: 0

摘要

激光技术的进步使得紧凑的太瓦激光系统具有高强度(I 0≥1018 W/cm2),适中的能量(≤100 J)和短脉冲(τl≤1 ps)成为可能。在超高强度下,激光与电子的相互作用变得高度非线性和相对论性,从而产生了各种各样新的和有趣的现象[1-5]。这些现象包括:(i)激光激发大振幅等离子体波(尾流场)[1,3-5],(ii)等离子体对激光脉冲的相对论性光引导[2-5],以及(iii)预制等离子体通道的光引导[5]。本文简要讨论了这些现象,包括自洽的二维轴对称模拟。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Intense Laser Pulse Propagation and Wakefield Generation in Plasma
Advances in laser technology have made possible compact terawatt laser systems with high intensities (I 0 ≥ 1018 W/cm2), modest energies (≤ 100 J) and short pulses (τl ≤ 1 ps). At ultra-high intensities, the laser-electron interaction becomes highly nonlinear and relativistic, thus resulting in a wide variety of new and interesting phenomena [1-5]. These phenomena include: (i) laser excitation of large amplitude plasma waves (wakefields) [1,3-5], (ii) relativistic optical guiding of laser pulses by plasmas [2-5], and (iii) optical guiding by preformed plasma channels [5]. This paper briefly discusses the these phenomena, including self-consistent, 2D-axisymmetric simulations.
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