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Strongly coupled large-angle stimulated Raman scattering of short laser pulse in plasma-filled capillary

机译:等离子体填充毛细管中短激光脉冲的强耦合大角度受激拉曼散射

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摘要

Strongly coupled large-angle stimulated Raman scattering (LA SRS) of a short intense laser pulse develops in a plane plasma-filled capillary differently than in a plasma with open boundaries. Coupling the laser pulse to a capillary seeds the LA SRS in the forward direction (scattering angle smaller than pi/2) and can thus produce a high instability level in the vicinity of the entrance plane. In addition, oblique mirror reflections off capillary walls partly suppress the lateral convection of scattered radiation and increase the growth rate of the SRS under arbitrary (not too small) angle. Hence, the saturated convective gain falls with an angle much slower than in an unbounded plasma and even for the near-forward SRS can be close to that of the direct backscatter. At a large distance, the LA SRS evolution in the interior of the capillary is dominated by quasi-one-dimensional leaky modes whose damping is related to the leakage of scattered radiation through the walls. (c) 2005 American Institute of Physics.
机译:短的强激光脉冲的强耦合大角度激发拉曼散射(LA SRS)在平面等离子体填充的毛细管中的发展不同于在具有开放边界的等离子体中的发展。将激光脉冲耦合到毛细管上会沿向前方向(散射角小于pi / 2)播种LA SRS,因此会在入射平面附近产生较高的不稳定性。另外,从毛细管壁上倾斜的镜面反射部分抑制了散射辐射的横向对流,并在任意(不太小)角度下增加了SRS的生长速率。因此,饱和对流增益的下降角度要比无边界等离子体中的下降慢得多,即使对于近前SRS也可以接近直接后向散射。在较远的距离上,毛细管内部的LA SRS演化主要由准一维泄漏模式控制,该泄漏模式的阻尼与散射辐射通过壁的泄漏有关。 (c)2005年美国物理研究所。

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