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Nonlinear analysis of relativistic harmonic generation by intense lasers in plasmas

机译:等离子体中强激光产生相对论谐波的非线性分析

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摘要

A linearly polarized, ultraintense laser field induces transverse plasma currents which are highly relativistic and nonlinear, resulting in the generation of coherent harmonic radiation in the forward direction (i.e., copropagating with the incident laser field). A nonlinear cold fluid model, valid for ultrahigh intensities, is formulated and used to analyze relativistic harmonic generation. The plasma density response is included self-consistently and is shown to significantly reduce the current driving the harmonic radiation. Phase detuning severely limits the growth of the harmonic radiation. The effects of diffraction are considered in the mildly relativistic limit. No third-harmonic signal emerges from a uniform plasma of near-infinite extent. A finite third-harmonic signal requires the use of a semi-infinite or finite slab plasma. For an initially uniform plasma, no second-harmonic radiation is generated. Generation of even harmonics requires transverse gradients in the initial plasma density profile.
机译:线性极化的超强激光场会感应出高度相对论和非线性的横向等离子体电流,从而导致在正向方向上产生相干谐波辐射(即与入射激光场共同传播)。建立了适用于超高强度的非线性冷流体模型,并将其用于分析相对论谐波的产生。等离子体密度响应可以自洽地包含在内,并且可以显着降低驱动谐波辐射的电流。相位失谐严重限制了谐波辐射的增长。相对于相对论,衍射的影响被认为是适度的。几乎无限远的均匀等离子体不会出现三次谐波信号。有限的三次谐波信号需要使用半无限或有限的平板等离子体。对于最初均匀的等离子体,不会产生二次谐波辐射。偶次谐波的产生需要初始等离子体密度分布中的横向梯度。

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