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作 者:Feili Wang Cibo Lou Yi Liang 王飞利;楼慈波;梁毅(Institute of Photonics,Faculty of Science,Ningbo University,Ningbo 315211,China;Guangxi Key Laboratory for Relativistic Astrophysics,School of Physics Science and Technology,Guangxi University,Nanning 530004,China)
机构地区:[1]Institute of Photonics,Faculty of Science,Ningbo University,Ningbo 315211,China [2]Guangxi Key Laboratory for Relativistic Astrophysics,School of Physics Science and Technology,Guangxi University,Nanning 530004,China [3]Corresponding author:loucibo@nbu.edu.cn [4]corresponding author: liangyi@gxu.edu.cn
出 处:《Chinese Optics Letters》2018年第11期9-13,共5页中国光学快报(英文版)
基 金:supported by the National Natural Science Foundation of China(No.11604058);Ningbo Natural Science Foundation(No.ZX2015000617);the K.C.Wong Magna Fund in Ningbo University,China;the Natural Science Foundation of Guangxi Province(No.2016GXNSFBA380244,2015GXNSFBA139011)
摘 要:We numerically investigate the propagation properties of ring Airy Gaussian beams (RAGBs) with cosine modulated optical vortices (CMOV). In comparison to the common RAGBs without any modulation, the dynamic propagation of RAGBs with CMOV exhibits a unique feature: the rings of RAGBs with CMOV will gradually shrink into several main lobes with the increase of the propagation distance. The number of lobes and the peak intensity of each lobe are determined by the factors of cosine modulated function. By designing the initial phase, we can easily change the transversal location of the peak intensity. Our results may find potential applications in optical manipulations.We numerically investigate the propagation properties of ring Airy Gaussian beams (RAGBs) with cosine modulated optical vortices (CMOV). In comparison to the common RAGBs without any modulation, the dynamic propagation of RAGBs with CMOV exhibits a unique feature: the rings of RAGBs with CMOV will gradually shrink into several main lobes with the increase of the propagation distance. The number of lobes and the peak intensity of each lobe are determined by the factors of cosine modulated function. By designing the initial phase, we can easily change the transversal location of the peak intensity. Our results may find potential applications in optical manipulations.
关 键 词:Airy beams MODULATION Optical potentials Optical vortices
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