Spiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma
The explicit expression of orbital angular momentum (OAM) spiral spectrum of Laguerre-Gaussian (LG) beam propagating in anisotropic plasma turbulence is derived based on Rytov theory. The relationship between the detection probability of OAM and the crosstalk with the anisotropy parameters, topologi...
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2021
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oai:doaj.org-article:30f56e1ad7b3453cad446759c0731cc52021-11-09T00:00:08ZSpiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma1943-065510.1109/JPHOT.2021.3119337https://doaj.org/article/30f56e1ad7b3453cad446759c0731cc52021-01-01T00:00:00Zhttps://ieeexplore.ieee.org/document/9568711/https://doaj.org/toc/1943-0655The explicit expression of orbital angular momentum (OAM) spiral spectrum of Laguerre-Gaussian (LG) beam propagating in anisotropic plasma turbulence is derived based on Rytov theory. The relationship between the detection probability of OAM and the crosstalk with the anisotropy parameters, topological charge, radial index, wavelength, beam width, receiving aperture, inner and outer scales are discussed in detail. In order to quantify the effect of plasma turbulence, we compared it with atmospheric turbulence based on restriction function. To optimize OAM detection probability, we also compared the effects of circular aperture method (CAM) with focusing mirror method (FMM) on the propagation characteristics of the spiral spectrum. The results show that even in the strong turbulence region of atmospheric turbulence, the radial dimension of LG beam in plasma turbulence is nearly twice that of atmospheric turbulence and the modes crosstalk has almost reached its upper bound. Besides, by comparing the two optimization methods, we found the ability to reduce crosstalk is related to the choice of beam width and receiving aperture. Therefore, we give a method to optimally select between the CAM and the FMM. We found the corresponding relationship and gave an analytical formula. The FMM has a greater ability to reduce crosstalk than the CAM when the beam width ≥4 cm and the aperture ≥3 cm. We quantified the effect of plasma turbulence and provide a guideline for the selection of beam width and receiving aperture under these two optimization methods. The research results may be helpful in the field of optical communication.Yankun WangLu BaiDanmeng ZhangJinyu XieYa GuoLixin GuoIEEEarticleOrbital angular momentumspiral spectrumanisotropic turbulenceApplied optics. PhotonicsTA1501-1820Optics. LightQC350-467ENIEEE Photonics Journal, Vol 13, Iss 6, Pp 1-10 (2021) |
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Orbital angular momentum spiral spectrum anisotropic turbulence Applied optics. Photonics TA1501-1820 Optics. Light QC350-467 |
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Orbital angular momentum spiral spectrum anisotropic turbulence Applied optics. Photonics TA1501-1820 Optics. Light QC350-467 Yankun Wang Lu Bai Danmeng Zhang Jinyu Xie Ya Guo Lixin Guo Spiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma |
description |
The explicit expression of orbital angular momentum (OAM) spiral spectrum of Laguerre-Gaussian (LG) beam propagating in anisotropic plasma turbulence is derived based on Rytov theory. The relationship between the detection probability of OAM and the crosstalk with the anisotropy parameters, topological charge, radial index, wavelength, beam width, receiving aperture, inner and outer scales are discussed in detail. In order to quantify the effect of plasma turbulence, we compared it with atmospheric turbulence based on restriction function. To optimize OAM detection probability, we also compared the effects of circular aperture method (CAM) with focusing mirror method (FMM) on the propagation characteristics of the spiral spectrum. The results show that even in the strong turbulence region of atmospheric turbulence, the radial dimension of LG beam in plasma turbulence is nearly twice that of atmospheric turbulence and the modes crosstalk has almost reached its upper bound. Besides, by comparing the two optimization methods, we found the ability to reduce crosstalk is related to the choice of beam width and receiving aperture. Therefore, we give a method to optimally select between the CAM and the FMM. We found the corresponding relationship and gave an analytical formula. The FMM has a greater ability to reduce crosstalk than the CAM when the beam width ≥4 cm and the aperture ≥3 cm. We quantified the effect of plasma turbulence and provide a guideline for the selection of beam width and receiving aperture under these two optimization methods. The research results may be helpful in the field of optical communication. |
format |
article |
author |
Yankun Wang Lu Bai Danmeng Zhang Jinyu Xie Ya Guo Lixin Guo |
author_facet |
Yankun Wang Lu Bai Danmeng Zhang Jinyu Xie Ya Guo Lixin Guo |
author_sort |
Yankun Wang |
title |
Spiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma |
title_short |
Spiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma |
title_full |
Spiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma |
title_fullStr |
Spiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma |
title_full_unstemmed |
Spiral Spectrum of a Laguerre-Gaussian Beam Propagating in Anisotropic Turbulent Plasma |
title_sort |
spiral spectrum of a laguerre-gaussian beam propagating in anisotropic turbulent plasma |
publisher |
IEEE |
publishDate |
2021 |
url |
https://doaj.org/article/30f56e1ad7b3453cad446759c0731cc5 |
work_keys_str_mv |
AT yankunwang spiralspectrumofalaguerregaussianbeampropagatinginanisotropicturbulentplasma AT lubai spiralspectrumofalaguerregaussianbeampropagatinginanisotropicturbulentplasma AT danmengzhang spiralspectrumofalaguerregaussianbeampropagatinginanisotropicturbulentplasma AT jinyuxie spiralspectrumofalaguerregaussianbeampropagatinginanisotropicturbulentplasma AT yaguo spiralspectrumofalaguerregaussianbeampropagatinginanisotropicturbulentplasma AT lixinguo spiralspectrumofalaguerregaussianbeampropagatinginanisotropicturbulentplasma |
_version_ |
1718441373968891904 |