激光束通过原子蒸汽传播的不稳定性

R. Boyd, D. Gauthier, M. S. Malcuit
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引用次数: 0

摘要

当激光在非线性光学介质中传播时,有几种非线性光学过程会导致光束不稳定。例如,自聚焦效应可以导致激光束中新的空间频率成分的增长。激光束对于新光谱成分的生长也是不稳定的。受激拉曼散射是导致这种不稳定性的一个众所周知的例子。在本文中,我们提出了一系列实验的结果,这些实验的结果是关于激光束通过原子蒸汽传播的情况下发生的一些不同的不稳定性。我们发现,当入射激光的频率接近于原子的单光子或双光子共振的频率时,这些不稳定性变得特别明显。在这两种情况下,我们都发现激光束对新频率分量的增长是不稳定的,并且这些新频率通常不会与入射激光共线发射。这些不稳定性很重要,因为它们限制了可用于驱动非线性光学过程的激光强度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Instabilities in the Propagation of Laser Beams Through Atomic Vapors
There are several nonlinear optical processes that can lead to instabilities in a laser beam as it propagates through a nonlinear optical medium. Self focusing effects, for instance, can lead to the growth of new spatial frequency components in a laser beam. A laser beam can also be unstable to the growth of new spectral components. Stimulated Raman scattering is a well-known example of a process that can lead to this sort of instability. In this paper, we present the results of a series of experiments on the somewhat different instabilities that occur for the case of the propagation of a laser beam through an atomic vapor. We find that these instabilities become particularly pronounced when the frequency of the incident laser is near to that of a one- or two-photon resonance of the atom. In either case, we find that the laser beam is unstable to the growth of new frequency components, and that in general these new frequencies are not emitted collinearly with the incident laser. These instabilities are important because they place a limit on the laser intensity that can be used to drive nonlinear optical processes.
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