| FUNDAMENTAL AREAS OF PHENOMENOLOGY(INCLUDING APPLICATIONS) |
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Nonlinear Generation of Perfect Vector Beams in Ultraviolet Wavebands |
| Hui Li1,2†, Haigang Liu2†, Yangfeifei Yang2, Ruifeng Lu1*, and Xianfeng Chen2,3,4,5* |
1Institute of Ultrafast Optical Physics, Department of Applied Physics & MIIT Key Laboratory of Semiconductor Microstructure and Quantum Sensing, Nanjing University of Science and Technology, Nanjing 210094, China
2State Key Laboratory of Advanced Optical Communication Systems and Networks, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
3Shanghai Research Center for Quantum Sciences, Shanghai 201315, China
4Jinan Institute of Quantum Technology, Jinan 250101, China
5Collaborative Innovation Center of Light Manipulations and Applications, Shandong Normal University, Jinan 250358, China
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| Cite this article: |
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Hui Li, Haigang Liu, Yangfeifei Yang et al 2022 Chin. Phys. Lett. 39 034201 |
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Abstract Perfect vector beams are a class of special vector beams with invariant radius and intensity profiles under changing topological charges. However, with the limitation of current devices, the generation of these vector beams is limited in the visible and infrared wavebands. Herein, we generate perfect vector beams in the ultraviolet region assisted by nonlinear frequency conversion. Experimental and simulation results show that the radius of the generated ultraviolet perfect vector beams remains invariant and is thus independent of the topological charge. Furthermore, we measure the power of the generated ultraviolet perfect vector beams with the change of their topological charges. This study provides an alternative approach to generating perfect vector beams for ultraviolet wavebands and may promote their application to optical trapping and optical communication.
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Received: 25 November 2021
Editors' Suggestion
Published: 01 March 2022
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| PACS: |
42.65.-k
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(Nonlinear optics)
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42.65.Ky
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(Frequency conversion; harmonic generation, including higher-order harmonic generation)
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42.25.Ja
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(Polarization)
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