Harmonic Generation by an Intense Picosecond Laser in an Underdense Plasma

X. Liu, J. Coe, C. Chien, D. Umstadter
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引用次数: 4

Abstract

Modest power lasers interacting with a neutral gas have been observed to produce coherent harmonic radiation (up to the 61 st harmonic) at odd multiples of the fundamental laser frequency[1]. This is a result of the laser field causing the bound electrons to oscillate in the anharmonic atomic potential. The process is limited to relatively low powers since increasing the fundamental laser power leads to ionization of the gas and to the production of unbound electrons. A very high-power laser interacting with a fully ionized plasma, however, may lead to the generation of large levels of coherent radiation at high harmonics (including even harmonics) of the incident laser frequency based on an entirely new mechanism. If the laser pulse is sufficiently intense, the plasma electron mass becomes modulated because of nonlinear relativistic effects [2]. We describe in this paper the theory and some experiments in which we observe signatures of this mechanism.
低密度等离子体中强皮秒激光的谐波产生
中等功率激光器与中性气体的相互作用已经被观察到产生相干谐波辐射(高达61 st谐波)在奇倍的基本激光频率[1]。这是激光场引起束缚电子在非调和原子势中振荡的结果。这个过程被限制在相对较低的功率,因为增加基本激光功率会导致气体电离并产生非束缚电子。然而,基于一种全新的机制,一个非常高功率的激光与完全电离的等离子体相互作用,可能导致在入射激光频率的高次谐波(包括偶数次谐波)下产生高水平的相干辐射。如果激光脉冲足够强,等离子体电子质量会因非线性相对论效应而发生调制[2]。本文描述了这一机制的理论和一些实验。
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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