Laser-triggered THz emission from near critical density targets

V. Yu. Bychenkov, A. V. Brantov, M. G. Lobok, A. S. Kuratov
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Abstract

Femtosecond laser pulse propagation in a relativistic self-trapping regime (RST) in a near-critical density plasma makes it possible to maximize the total charge of the accelerating electrons and laser-to-electrons conversion rate, that can be used to provide a large amount of the THz range coherent transition radiation. The three-dimensional particle-in-cell simulations demonstrate how such transition radiation generates when electrons escape into vacuum either from the low-density target itself, or after passing through a thin foil located at the target end. Advantage of the RST regime for generation of THz pulses is clearly demonstrated as compared to laser irradiation of such a standard target as a foil with preplasma on its front side. Simulation performed has shown that for the optimized laser-target matching a 2-J femtosecond laser pulse is able to produce quasi-unipolar Thz pulses with energy exceeding 100 mJ.
近临界密度目标的激光触发太赫兹发射
飞秒激光脉冲在近临界密度等离子体中的相对论自俘获机制(RST)中传播,使得加速电子的总电荷量和激光-电子转换率最大化成为可能,从而可用于提供大量太赫兹范围的相干过渡辐射。三维粒子入室模拟演示了当电子从低密度靶本身逸出进入真空或穿过靶端薄泡沫后,如何产生这种过渡辐射。与激光照射前端带有预等离子体的箔片这样的标准靶相比,RST 系统在产生 THz 脉冲方面的优势得到了清楚的证明。模拟结果表明,在优化的激光-靶匹配条件下,2 Jemtosecond 激光脉冲能够产生能量超过 100 mJ 的准单极 THz 脉冲。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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