超短激光激发的高振幅表面等离子体波中的电子加速

J. Kupersztych, M. Raynaud, C. Riconda
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引用次数: 0

摘要

我们研究了一种在锐边超密等离子体中激光激发表面等离子体波共振场加速产生相对论性电子的新机制。这种机制是将最近在短脉冲激光金属相互作用中观察到的一种效应推广到高强度激光场。众所周知,在激光脉冲的上升时间内,p偏振激光撞击结构金属表面会产生等离子体,其温度可达到数百电子伏特。如果脉冲持续时间(<~ 100 fs)使电子与表面等离子体波的相互作用在流体动力膨胀有时间平滑等离子体密度尖锐边缘之前发生,则可以满足激光共振激发表面等离子体波的条件。我们发现,在这种情况下,位于等离子体表面附近的强非均匀增强电场可能会加速电子向真空方向运动,这一机制的效率取决于两个特征长度之间的比率RL:真空中表面波场的延伸长度和高频高振幅场中粒子覆盖的典型距离。我们发现了一个单位数量级的RL的最佳状态,在这种情况下,电子可以在表面等离子体波的增强场中加速到高频动量posc的数量级。给出了一维相对论测试粒子模拟电子与等离子体波场相互作用的结果。特别是,我们表明,当激光强度达到1018W/cm2数量级时,某些MeV的电子能量可以达到。对最佳情况下得到的电子能量分布函数进行了数值计算。由于加速电子所经历的等离子体波场的相位依赖,光谱显示出一个明确的峰结构。这项研究提出了一种新的可能性的大电流高能脉冲电子源。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electron acceleration in high-amplitude surface plasma waves excited by ultrashort laser
We have investigated a new mechanism for creation of relativistic electrons via the acceleration by the resonant field of laser excited surface plasma waves in sharp-edged overdense plasmas. This mechanism consists in a generalization to high-intensity laser fields of an effect recently observed in the context of short-pulse laser metal interaction. As it is well known, a p-polarized laser impinging onto a structured metal surface creates a plasma during the rise time of the laser pulse, which can reach temperatures of several hundreds of eV. If the pulse duration (<~ 100 fs) is such that the interaction of the electrons with the surface plasma wave occurs before the hydrodynamic expansion has time to smooth the plasma density sharp edge, the conditions for resonant excitation of surface plasma waves by the laser can be fulfilled. We show that in this case the strongly inhomogeneous enhanced electric field located near the plasma surface may accelerate the electrons toward the vacuum, the efficiency of this mechanism depending on the ratio RL between two characteristic lengths: the extension length of the surface wave field in the vacuum and the typical distance covered by the particles in the high-frequency high-amplitude field. We find an optimum regime for RL of the order of unity, in which case the electrons can be accelerated up to a momentum of the order of magnitude of the high-frequency momentum posc in the enhanced field of the surface plasma wave. The results of a 1D relativistic test-particle simulation modeling the interaction of the electrons with the plasma wave field are presented. In particular, we show that electron energies of some MeV may be reached for laser intensities of the order of 1018W/cm2. The resulting electron energy distribution function is numerically calculated for the optimum case. The spectrum shows a well-defined peaked structure due to the dependence on the phase of the plasma wave field experienced by the accelerated electrons. This study suggests a novel possibility of high-current energetic pulsed electron sources.
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