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径向极化涡旋光束紧聚焦中的自旋轨道霍尔效应。

Spin-orbit Hall effect in the tight focusing of a radially polarized vortex beam.

作者信息

Li Hehe, Ma Chenghao, Wang Jingge, Tang Miaomiao, Li Xinzhong

出版信息

Opt Express. 2021 Nov 22;29(24):39419-39427. doi: 10.1364/OE.443271.

Abstract

When the first-order radially polarized vortex beam propagates in an uniaxial crystal, the spin and the orbital angular momentum parts can be separated. It is called the optical spin-orbit Hall effect. In this study, we investigate the tight focusing of the radially polarized vortex beam theoretically and find the spatial separation of the spin and the orbital angular momentum parts occurs in the focal plane when the polarization order equals 1 and the vortex charge equals 1 (or -1). Moreover, when the initial phase of the polarization state takes π/2, the spatial separation of intensity in the focal plane corresponds to the spatial separation of the spin and the orbital angular momentum parts. This phenomenon can be considered as a manifestation of the optical spin-orbit Hall effect in the tight focusing of radially polarized vortex beam. Also, we show that, when the polarization order is greater than 1, the initial phase change of polarization state just leads to the rotation of the focal field and the spin and the orbital angular momentum density in the focal plane. Our results provide the potential application in the field of optical micro-manipulation.

摘要

当一阶径向偏振涡旋光束在单轴晶体中传播时,自旋和轨道角动量部分可以分离。这被称为光学自旋 - 轨道霍尔效应。在本研究中,我们从理论上研究了径向偏振涡旋光束的紧聚焦,发现当偏振阶数等于1且涡旋电荷等于1(或 -1)时,自旋和轨道角动量部分在焦平面上会发生空间分离。此外,当偏振态的初始相位为π/2时,焦平面上强度的空间分离对应于自旋和轨道角动量部分的空间分离。这种现象可以被视为光学自旋 - 轨道霍尔效应在径向偏振涡旋光束紧聚焦中的一种表现。同时,我们表明,当偏振阶数大于1时,偏振态的初始相位变化仅导致焦场以及焦平面上自旋和轨道角动量密度的旋转。我们的结果为光学微操纵领域提供了潜在应用。

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