Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere Beam

In this paper, the far-field topological structures (FFTSs) of the second harmonic (SH) from higher-order Poincaré sphere (HOPS) beams, including circularly polarized vortex beams (VBs), cylindrically vector beams (CVBs) and elliptically polarized CVBs (EPCVBs), were demonstrated and reported. To be...

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Main Authors: Yangyang Li, Ziping Zhu, Yuanxiang Wang, Jiantai Dou, Li Fan, Bo Li, Youyou Hu
Format: Article
Language:English
Published: MDPI AG 2025-04-01
Series:Photonics
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Online Access:https://www.mdpi.com/2304-6732/12/5/407
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author Yangyang Li
Ziping Zhu
Yuanxiang Wang
Jiantai Dou
Li Fan
Bo Li
Youyou Hu
author_facet Yangyang Li
Ziping Zhu
Yuanxiang Wang
Jiantai Dou
Li Fan
Bo Li
Youyou Hu
author_sort Yangyang Li
collection DOAJ
description In this paper, the far-field topological structures (FFTSs) of the second harmonic (SH) from higher-order Poincaré sphere (HOPS) beams, including circularly polarized vortex beams (VBs), cylindrically vector beams (CVBs) and elliptically polarized CVBs (EPCVBs), were demonstrated and reported. To begin with, the hidden FFTSs of the SH after propagating the twice Rayleigh range were simulated based on the vectorial coupled wave equations and the Collins formula. Then, the experimental setup was established to achieve the SH from the HOPS by applying two orthogonal 5% MgO: PPLN crystals, the FFTSs of which were demonstrated. The theoretical and experimental results indicate that for the circularly polarized VBs, the FFTSs of the SH still exhibit the 135°-linearly polarized VBs, which is similar to that of the SH in-source plane, because the SH is the eigen-mode of free space, while for the CVBs, the FFTSs of the SH generally show the disappearance of the central dark core, replaced by the maximum light intensity at the center due to the topological phase transition during propagation. Especially of note, for the EPCVBs, the FFTSs of the SH display the maximum light intensity at the center, but the FFTSs in the horizontal and vertical directions reveal rotational symmetry related to the chirality of the EPCVBs. The results reveal the evolution mechanisms of the SH from the HOPS in the far field, which may facilitate the applications of the SH from HOPS beam.
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spelling doaj-art-4e6466a77e3446959e1ce4a3e3a8b0bb2025-08-20T03:14:42ZengMDPI AGPhotonics2304-67322025-04-0112540710.3390/photonics12050407Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere BeamYangyang Li0Ziping Zhu1Yuanxiang Wang2Jiantai Dou3Li Fan4Bo Li5Youyou Hu6School of Science, Jiangsu University of Science and Technology, Zhenjiang 212100, ChinaSchool of Science, Jiangsu University of Science and Technology, Zhenjiang 212100, ChinaSchool of Science, Jiangsu University of Science and Technology, Zhenjiang 212100, ChinaSchool of Science, Jiangsu University of Science and Technology, Zhenjiang 212100, ChinaCollege of Physics Science and Technology, Institute of Applied Photonic Technology, Yangzhou University, Yangzhou 225002, ChinaSchool of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan 430074, ChinaSchool of Science, Jiangsu University of Science and Technology, Zhenjiang 212100, ChinaIn this paper, the far-field topological structures (FFTSs) of the second harmonic (SH) from higher-order Poincaré sphere (HOPS) beams, including circularly polarized vortex beams (VBs), cylindrically vector beams (CVBs) and elliptically polarized CVBs (EPCVBs), were demonstrated and reported. To begin with, the hidden FFTSs of the SH after propagating the twice Rayleigh range were simulated based on the vectorial coupled wave equations and the Collins formula. Then, the experimental setup was established to achieve the SH from the HOPS by applying two orthogonal 5% MgO: PPLN crystals, the FFTSs of which were demonstrated. The theoretical and experimental results indicate that for the circularly polarized VBs, the FFTSs of the SH still exhibit the 135°-linearly polarized VBs, which is similar to that of the SH in-source plane, because the SH is the eigen-mode of free space, while for the CVBs, the FFTSs of the SH generally show the disappearance of the central dark core, replaced by the maximum light intensity at the center due to the topological phase transition during propagation. Especially of note, for the EPCVBs, the FFTSs of the SH display the maximum light intensity at the center, but the FFTSs in the horizontal and vertical directions reveal rotational symmetry related to the chirality of the EPCVBs. The results reveal the evolution mechanisms of the SH from the HOPS in the far field, which may facilitate the applications of the SH from HOPS beam.https://www.mdpi.com/2304-6732/12/5/407second harmonicfar-field topological structureshigher-order Poincaré sphere beams
spellingShingle Yangyang Li
Ziping Zhu
Yuanxiang Wang
Jiantai Dou
Li Fan
Bo Li
Youyou Hu
Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere Beam
Photonics
second harmonic
far-field topological structures
higher-order Poincaré sphere beams
title Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere Beam
title_full Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere Beam
title_fullStr Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere Beam
title_full_unstemmed Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere Beam
title_short Far-Field Topological Structure of the Second Harmonic from Higher-Order Poincaré Sphere Beam
title_sort far field topological structure of the second harmonic from higher order poincare sphere beam
topic second harmonic
far-field topological structures
higher-order Poincaré sphere beams
url https://www.mdpi.com/2304-6732/12/5/407
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