在PALS装置相互作用实验中观察到的固体激光脉冲后坑形成

I. Y. Doskach, S. Gus'kov, K. Jungwirth, M. Kalal, A. Kasperczuk, B. Králiková, E. Krouský, J. Limpouch, K. Mašek, M. Pfeifer, T. Pisarczyk, K. Rohlena, V. Rozanov, J. Skála, J. Ullschmied
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引用次数: 5

摘要

报道了PALS装置激光与大质量铝靶相互作用实验的结果。主要研究了激光脉冲能量(100j ~ 600j)、强度(1013 W/cm2 ~ 1015 W/cm2)、波长(0.438 μm ~ 1.315 μm)、聚焦光束半径(35 μm ~ 600 μm)等不同激光脉冲作用下的弹坑形成。陨石坑的复制品是用蜡制成的,它们的深度和半径随后通过显微镜测量得到。激光脉冲引发的冲击波传播到目标的持续时间比激光脉冲本身的传播时间(400 ps)长得多。这是实验安排的一个重要特点。提出了激光脉冲结束后冲击波在固体中传播衰减形成脉冲后弹坑的理论模型,并应用该模型对实验结果进行了解释。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Laser-produced post-pulse crater formation in solids observed in PALS facility interaction experiment
Results from PALS facility laser-massive Al target interaction experiments are reported. Main attention is devoted craters formation under the action of laser pulses of various energy (from 100 J up to 600 J), intensity (from 1013 W/cm2 up to 1015 W/cm2), laser wavelength (0.438 μm and 1.315 μm), and focal beam radius (from 35 μm up to 600 μm). Crater replicas were made of wax and their depths and radii were subsequently obtained by microscopy measurements. Duration of the laser-pulse-initiated shock wave propagation into the targets was much longer than that of the laser pulse itself (400 ps). This was an important feature of the experimental arrangement. Theoretical model of the post-pulse crater formation by the shock wave propagating and decaying in solids after the end of the laser pulse is presented and applied for explanation of the results obtained in experiments.
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