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Electron kinetic simulations of solid density Al plasmas produced by intense subpicosecond laser pulses. I. Ionization dynamics in 30 femtosecond pulses

机译:强亚皮秒激光脉冲产生的固体密度Al等离子体的电子动力学模拟。 I. 30飞秒脉冲中的电离动力学

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The interaction of a 10(18) W/cm(2), 30 fs laser pulse with solid Al was simulated with the electron kinetic code "FPI" [J. P. Matte , Phys. Rev. Lett. 72, 1208 (1994)] in which an improved average ion module was fully coupled to the electron kinetics. It includes electron impact ionization and excitation and their inverse processes: collisional recombination and de-excitation; as well as radiative decay and pressure ionization. We compare to runs without the inverse processes, and also without atomic physics (with set to 11). Atomic physics strongly affects the energy balance and the shape of the distribution function. Line radiation is mostly due to three body recombination into excited states after the peak of the pulse, as the plasma cools down. Despite the atomic processes and the high density, strongly non-Maxwellian distribution functions were obtained due to very steep temperature gradients and strong collisional heating, at the peak of the pulse. However, after the pulse, there is a very rapid thermalization of the electron distribution to which inverse processes strongly contribute. (C) 2001 American Institute of Physics. [References: 58]
机译:用电子动力学代码“ FPI”模拟了10(18)W / cm(2),30 fs的激光脉冲与固体Al的相互作用。 P. Matte,物理学。牧师72,1208(1994)],其中改进的平均离子模块完全与电子动力学耦合。它包括电子碰撞的电离和激发以及它们的逆过程:碰撞重组和去激发;以及辐射衰减和压力电离。我们将运行与没有逆过程,也没有原子物理学(设置为11)的运行进行比较。原子物理学极大地影响能量平衡和分布函数的形状。线辐射主要是由于等离子冷却后,三个主体在脉冲峰值后重新组合成激发态。尽管存在原子过程和高密度,但由于在脉冲峰值处非常陡峭的温度梯度和强烈的碰撞加热,仍获得了强烈的非麦克斯韦分布函数。但是,在脉冲之后,电子分布会非常快速地热化,逆过程对此有很大的作用。 (C)2001美国物理研究所。 [参考:58]

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