受激康普顿后向散射和高强度Kapitza-Dirac效应*

D. Schumacher, P. Bucksbaum, M. Bashkansky
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引用次数: 0

摘要

我们报道了低能量自由电子在强度为1013至1014W/cm2.1的光驻波中的散射,这种相互作用是Kapitza-Dirac效应的高强度极限,其中电子从驻波“晶格”散射。在这种情况下,交换的动量超过倒易晶格矢量500倍或更多,散射率与光学频率相当。电子的运动最容易用经典力学来分析。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Stimulated Compton Backscattering and the High Intensity Kapitza-Dirac Effect*
We report the scattering of low energy free electrons from an optical standing wave at intensities of 1013 to 1014W/cm2.1 This interaction is the high intensity limit of the Kapitza-Dirac effect,2 wherein electrons Bragg scatter from the standing wave "lattice". In this regime, the momentum exchanged exceeds the reciprocal lattice vector by a factor of 500 or more, and the scattering rate is compar able to the optical frequency. The electron motion is most easily analyzed by classical mechanics.
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