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

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 b...

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Autores principales: Zheng, Guoliang, Wu, Qingyang, He, Tiefeng, Zhang, Xuhui
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9318936/
https://www.ncbi.nlm.nih.gov/pubmed/35888823
http://dx.doi.org/10.3390/mi13071006
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author Zheng, Guoliang
Wu, Qingyang
He, Tiefeng
Zhang, Xuhui
author_facet Zheng, Guoliang
Wu, Qingyang
He, Tiefeng
Zhang, Xuhui
author_sort Zheng, Guoliang
collection PubMed
description 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.
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spelling pubmed-93189362022-07-27 Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis Zheng, Guoliang Wu, Qingyang He, Tiefeng Zhang, Xuhui Micromachines (Basel) Article 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. MDPI 2022-06-26 /pmc/articles/PMC9318936/ /pubmed/35888823 http://dx.doi.org/10.3390/mi13071006 Text en © 2022 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Zheng, Guoliang
Wu, Qingyang
He, Tiefeng
Zhang, Xuhui
Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis
title Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis
title_full Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis
title_fullStr Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis
title_full_unstemmed Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis
title_short Propagation Characteristics of Circular Airy Vortex Beams in a Uniaxial Crystal along the Optical Axis
title_sort propagation characteristics of circular airy vortex beams in a uniaxial crystal along the optical axis
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9318936/
https://www.ncbi.nlm.nih.gov/pubmed/35888823
http://dx.doi.org/10.3390/mi13071006
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