Neural network classification of beams carrying orbital angular momentum after propagating through controlled experimentally generated optical turbulence
William A. Jarrett, Svetlana Avramov-Zamurovic, Joel M. Esposito, K. Peter Judd, and Charles Nelson
{"title":"Neural network classification of beams carrying orbital angular momentum after propagating through controlled experimentally generated optical turbulence","authors":"William A. Jarrett, Svetlana Avramov-Zamurovic, Joel M. Esposito, K. Peter Judd, and Charles Nelson","doi":"10.1364/josaa.515096","DOIUrl":null,"url":null,"abstract":"We generate an alphabet of spatially multiplexed Laguerre–Gaussian beams carrying orbital angular momentum, which are demultiplexed at reception by a convolutional neural network (CNN). In this investigation, a methodology for optimizing alphabet design for best classification rates is proposed, and three 256-symbol alphabets are designed for performance evaluation in optical turbulence. The beams were propagated in three environments: through underwater optical turbulence generated by Rayleigh–Bénard (RB) convection (<span><span style=\"color: inherit;\"><span><span><span style=\"margin-right: 0.05em;\"><span>C</span></span><span style=\"height: 1.86em; vertical-align: -0.64em;\"><span><span><span style=\"margin-bottom: -0.25em;\"><span><span>2</span></span></span></span></span><span><span><span style=\"margin-top: -0.85em;\"><span><span>n</span></span></span></span></span></span></span><span style=\"margin-left: 0.333em; margin-right: 0.333em;\">≅</span><span>1</span><span><span style=\"margin-right: 0.05em;\"><span>0</span></span><span style=\"vertical-align: 0.5em;\"><span>−</span><span>11</span></span></span><span style=\"width: 0.278em; height: 0em;\"></span><span><span style=\"margin-right: 0.05em;\"><span>m</span></span><span style=\"vertical-align: 0.5em;\"><span>−</span><span>2</span><span><span>/</span></span><span>3</span></span></span></span></span><span tabindex=\"0\"></span><script type=\"math/tex\">{C}_{n}^{2}\\cong 1{0}^{-11}\\;{\\rm m}^{-2/3}</script></span>), through a simulated propagation path derived from the Nikishov spectrum (<span><span style=\"color: inherit;\"><span><span><span style=\"margin-right: 0.05em;\"><span>C</span></span><span style=\"height: 1.86em; vertical-align: -0.64em;\"><span><span><span style=\"margin-bottom: -0.25em;\"><span><span>2</span></span></span></span></span><span><span><span style=\"margin-top: -0.85em;\"><span><span>n</span></span></span></span></span></span></span><span style=\"margin-left: 0.333em; margin-right: 0.333em;\">≅</span><span>1</span><span><span style=\"margin-right: 0.05em;\"><span>0</span></span><span style=\"vertical-align: 0.5em;\"><span>−</span><span>13</span></span></span><span style=\"width: 0.278em; height: 0em;\"></span><span><span style=\"margin-right: 0.05em;\"><span>m</span></span><span style=\"vertical-align: 0.5em;\"><span>−</span><span>2</span><span><span>/</span></span><span>3</span></span></span></span></span><span tabindex=\"0\"></span><script type=\"math/tex\">{C}_{n}^{2}\\cong 1{0}^{-13}\\; {\\rm m}^{-2/3}</script></span>), and through optical turbulence from a thermal point source located in a water tank (<span><span style=\"color: inherit;\"><span><span><span style=\"margin-right: 0.05em;\"><span>C</span></span><span style=\"height: 1.86em; vertical-align: -0.64em;\"><span><span><span style=\"margin-bottom: -0.25em;\"><span><span>2</span></span></span></span></span><span><span><span style=\"margin-top: -0.85em;\"><span><span>n</span></span></span></span></span></span></span><span style=\"margin-left: 0.333em; margin-right: 0.333em;\">≅</span><span>1</span><span><span style=\"margin-right: 0.05em;\"><span>0</span></span><span style=\"vertical-align: 0.5em;\"><span>−</span><span>10</span></span></span><span style=\"width: 0.278em; height: 0em;\"></span><span><span style=\"margin-right: 0.05em;\"><span>m</span></span><span style=\"vertical-align: 0.5em;\"><span>−</span><span>2</span><span><span>/</span></span><span>3</span></span></span></span></span><span tabindex=\"0\"></span><script type=\"math/tex\">{C}_{n}^{2}\\cong 1{0}^{-10}\\;{\\rm m}^{-2/3}</script></span>). We report a classification accuracy of 93.1% for the RB environment, 99.99% in simulation, and 48.5% in the point source environment. The project demonstrates that the CNN can classify the complex alphabet symbols in a practical turbulent flow that exhibits strong optical turbulence, provided sufficient training data is available and testing data is representative of the specific environment. We find the most important factor in a high classification accuracy is a diversification in the intensity profiles of the alphabet symbols.","PeriodicalId":501620,"journal":{"name":"Journal of the Optical Society of America A","volume":"24 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-03-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the Optical Society of America A","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/josaa.515096","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
We generate an alphabet of spatially multiplexed Laguerre–Gaussian beams carrying orbital angular momentum, which are demultiplexed at reception by a convolutional neural network (CNN). In this investigation, a methodology for optimizing alphabet design for best classification rates is proposed, and three 256-symbol alphabets are designed for performance evaluation in optical turbulence. The beams were propagated in three environments: through underwater optical turbulence generated by Rayleigh–Bénard (RB) convection (C2n≅10−11m−2/3), through a simulated propagation path derived from the Nikishov spectrum (C2n≅10−13m−2/3), and through optical turbulence from a thermal point source located in a water tank (C2n≅10−10m−2/3). We report a classification accuracy of 93.1% for the RB environment, 99.99% in simulation, and 48.5% in the point source environment. The project demonstrates that the CNN can classify the complex alphabet symbols in a practical turbulent flow that exhibits strong optical turbulence, provided sufficient training data is available and testing data is representative of the specific environment. We find the most important factor in a high classification accuracy is a diversification in the intensity profiles of the alphabet symbols.