Nonlinear propagation effects on high-power optical-vortex pulses in anisotropic crystals

Masato Suzuki, Y. Toda, R. Morita
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Abstract

Having a helical wavefront, a Laguerre-Gaussian (LG) mode or optical vortex is one of the modes of paraxial solutions to wave equation. The optical vortex has unique properties. The beam has a phase singularity on its center, which shows a dark part on its center of intensity profile, and carries an orbital angular momentum of light well defined by the topological charge ℓ [1]. These characteristics recently attracted much attention. For more versatile applications, high power optical-vortex pulses are desired. Typically, optical vortices are generated by using a spiral plate [2], a spatial light modulator (SLM) [3], a photonic-crystal axially-symmetric polarizer/waveplate [4] or a uniaxial crystal [5]. Among them, the most flexible method is by SLM. However, this method using SLM is power-limited owing to its damage threshold. Hence, as an alternative to generate high power optical-vortex pulses, we choose the method using a uniaxial crystal, which is rather flexible. In this scheme, the nonlinear effects have not been clarified in detail. In the present paper, we investigate nonlinear effects on optical-vortex pulse generation through the spin-orbit interaction and its propagation in an anisotropic crystal.
高功率光涡旋脉冲在各向异性晶体中的非线性传播效应
具有螺旋波前的Laguerre-Gaussian (LG)模式或光学涡旋是波动方程近轴解的一种模式。光学涡旋具有独特的性质。该光束在其中心有一个相位奇点,在其强度曲线的中心有一个暗部,并携带由拓扑电荷r[1]定义的光的轨道角动量。这些特点最近引起了人们的广泛关注。为了更广泛的应用,需要高功率光涡旋脉冲。通常,光学漩涡的产生是通过使用螺旋板[2]、空间光调制器(SLM)[3]、光子晶体轴对称偏振器/波片[4]或单轴晶体[5]。其中,最灵活的方法是SLM。然而,这种使用SLM的方法由于其损伤阈值而受到功率限制。因此,作为产生高功率光涡旋脉冲的一种替代方法,我们选择了使用单轴晶体的方法,它具有相当的灵活性。在这个方案中,非线性效应没有得到详细的阐明。本文研究了各向异性晶体中自旋-轨道相互作用对光涡旋脉冲产生及其传播的非线性影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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