Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis

被引:8
|
作者
Zheng, Guoliang [1 ]
Wu, Qingyang [2 ]
He, Tiefeng [1 ]
Zhang, Xuhui [1 ]
机构
[1] Shenzhen Technol Univ, Sino German Coll Intelligent Mfg, Shenzhen 518118, Peoples R China
[2] Shenzhen Technol Univ, Coll Big Data & Internet, Shenzhen 518118, Peoples R China
基金
中国国家自然科学基金;
关键词
optical vortex; abruptly autofocusing beams; uniaxial crystal; spin-orbital coupling; ORBITAL ANGULAR-MOMENTUM; ELECTROMAGNETIC-FIELDS; DYNAMICS; LIGHT; GENERATION; SPIN; RADIATION;
D O I
10.3390/mi13071006
中图分类号
O65 [分析化学];
学科分类号
070302 ; 081704 ;
摘要
Circular airy vortex beams (CAVBs) have attracted much attention due to their "abruptly autofocusing" effect, phase singularity, and their potential applications in optical micromanipulation, communication, etc. In this paper, we numerically investigated the propagation properties of circular airy beams (CABs) imposed with different optical vortices (OVs) along the optical axis of a uniaxial crystal for the first time. Like other common beams, a left-hand circular polarized (LHCP) CAVB, propagating along the optical axis in a uniaxial crystal, can excite a right-hand circular polarized (RHCP) component superimposed with an on-axis vortex of topological charge (TC) number of 2. When the incident beam is an LHCP CAB imposed with an on-axis vortex of TC number of l = 1, both of the two components have an axisymmetric intensity distribution during propagation and form hollow beams near the focal plane because of the phase singularity. The phase pattern shows that the LHCP component carries an on-axis vortex of TC number of l = 1, while the RHCP component carries an on-axis vortex of TC number of l = 3. With a larger TC number (l = 3), the RHCP component has a larger hollow region in the focal plane compared to the LHCP component. We also studied cases of CABs imposed with one and two off-axis OVs. The off-axis OV makes the CAVB's profile remain asymmetric throughout the propagation. As the propagation distance increases, the off-axis OVs move near the center of the beam and overlap, resulting in a special intensity and phase distribution near the focal plane.
引用
收藏
页数:11
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