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1.中国科学院 西安光学精密机械研究所 a.光子网络技术研究室;b.瞬态国家重点实验室,西安 710119
2.中国科学院大学 未来技术学院,北京 101408
3.海洋石油工程股份有限公司安装分公司,天津 300461
韩笑天(1996-),男,陕西渭南人。博士,主要研究方向为水下无线光通信。
谢小平,研究员。E-mail:xxp@opt.ac.cn
纸质出版日期:2023-08-10,
收稿日期:2023-05-04,
修回日期:2023-05-16,
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韩笑天,廖佩璇,李鹏,等.蒙特卡洛法仿真激光在水下信道中的传输特性[J].光通信研究,2023(4):53-59.
Han X T, Liao P X, Li P, et al. Monte Carlo Simulation on Laser Transmission Characteristics in an Underwater Channel [J].Study on Optical Communications, 2023(4):53-59.
韩笑天,廖佩璇,李鹏,等.蒙特卡洛法仿真激光在水下信道中的传输特性[J].光通信研究,2023(4):53-59. DOI: 10.13756/j.gtxyj.2023.04.009.
Han X T, Liao P X, Li P, et al. Monte Carlo Simulation on Laser Transmission Characteristics in an Underwater Channel [J].Study on Optical Communications, 2023(4):53-59. DOI: 10.13756/j.gtxyj.2023.04.009.
针对海洋港湾海水强吸收和高散射的特性,文章利用蒙特卡洛方法仿真研究了激光在浑浊港湾海水中的传输特性。文章在一定的光波长、光能量和发散角下,量化分析了水质参数和传输距离对激光的功率、脉冲响应以及光斑质量的影响。研究结果表明,激光在浑浊港湾海水中传输时,随着衰减长度的增加,光功率的衰减特性保持一致,且光功率的衰减速度不符合比尔定律所描述的线性关系。在相同的水质条件下,光脉冲的宽度和光斑的尺寸随着传输距离的增加而增大,但是当传输距离从20个衰减长度传输至30个衰减长度时,光脉冲宽度基本不变,光脉冲展宽量的变化小于1 ns,此时光斑尺寸持续增大。另外,在相同的衰减长度处,光脉冲和光斑的展宽量随着水质衰减系数的增大而减小。
The transmission characteristics of laser in four types of harbor water were studied using Monte Carlo method simulations for the characteristics of strong absorption and high scattering of water in marine harbors. The effects of water quality parameters and transmission distance on the optical signal power
impulse response and spot quality were quantified and analyzed at certain optical wavelengths
optical energies and divergence angles. The analysis shows that the attenuation characteristics of laser remain consistent as the attenuation length increases when the optical signal is transmitted in the four types of harbor waters. The rate of attenuation of the optical power also does not conform to the linear relationship described by Beer's law. Under the same water quality conditions
the width of the optical pulse
the size of the light spot increases with the attenuation length. However
when the attenuation length is transmitted from 20 to 30
the width of the optical pulse is almost unchanged
and the change in the amount of light pulse spreading is less than 1 ns with the size of the light spot increases continuously. In addition
at the same attenuation length
the light pulse and the spreading amount of light spot with the water quality attenuation coefficient increases and decreases.
水下无线光传输蓝绿光蒙特卡洛脉冲响应光斑变化
underwater wireless optical transmissionbule-green lightMonto Carloimpulse responselight spot change
Cox W C. Simulation, Modeling, and Design of Underwater Optical Communication Systems[D]. North Carolina, US: North Carolina State University, 2012.
黄爱萍, 张莹珞, 陶林伟. 蒙特卡洛仿真的水下激光通信信道特性[J]. 红外与激光工程, 2017, 46(4): 219-224.
Huang A P, Zhang Y L, Tao L W. Monte Carlo Simulation on Channel Characteristics of Underwater Laser Communications[J]. Infrared and Laser Engineering, 2017, 46(4):219-224.
吴琼, 王博, 王涛, 等. 基于蒙特卡洛法的水下无线光传输特性分析[J]. 光子学报, 2021, 50(4):22-31.
Wu Q, Wang B, Wang T, et al. Analysis of Underwater Wireless Optical Transmission Characteristics based on Monte Carlo Method[J]. Acta Photonica Sinica, 2021, 50(4):22-31.
Qin J J, Fu M, Sun M N, et al. Simulation of Beam Characteristics in Long-distance Underwater Optical Communication[C]//Global Oceans 2020:Singapore-U.S.Gulf Coast. Biloxi, MS, USA:IEEE, 2020:9389218.
Jiang R, Sun C M, Zhang L, et al. Deep Learning Aided Signal Detection for SPAD-based Underwater Optical Wireless Communications[J]. IEEE Access, 2020, 8:20363-20374.
Zhang L, Tang X, Sun C M, et al. Over 10 Attenuation Length Gigabits per Second Underwater Wireless Optical Communication Using a Silicon Photomultiplier (SiPM) based Receiver[J]. Optics Express, 2020, 28(17):24968-24980.
Hu S Q, Mi L, Zhou T H, et al. 35.88 Attenuation Lengths and 3.32 bits/photon Underwater Optical Wireless Communication based on Photon-counting Receiver with 256-PPM[J]. Optics Express, 2018, 26(17): 21685-21699.
Mobley C, Gordon H, Kattawar W G, et al. Comparison of Numerical Models for Computing Underwater Light Fields[J]. Applied Optics, 1993, 32:7484-7504.
Sahu S K, Shanmugam P. A Study on the Effect of Scattering Properties of Marine Particles on Underwater Optical Wireless Communication Channel Characteristics[C]//OCEANS 2017.Aberdeen, UK:IEEE, 2017:8084720.
Gabriel C, Khalighi M A, Bourennane S, et al. Monte-Carlo-based Channel Characterization for Underwater Optical Communication Systems[J]. Journal of Optical Communications and Networking, 2013, 5(1):1-12.
Cox W, Muth J. Simulating Channel Losses in an Underwater Optical Communication System[J]. Journal of the Optical Society of America A, 2014, 31(5): 920-934.
Toublanc D. Henyey-greenstein and Mie Phase Functions in Monte Carlo Radiative Transfer Computations[J]. Applied Optics, 1996, 35(18):3270-3274.
Haltrin V I. One-parameter Two-term Henyey-greenstein Phase Function for Light Scattering in Seawater[J]. Applied Optics, 2002, 41(6):1022-1028.
Freda W, Piskozub J. Improved Method of Fournier-forand Marine Phase Function Parameterization[J]. Optics Express, 2007, 15(20):12763-12768.
Mobley C D, Sundman L K, Boss E. Phase Function Effects on Oceanic Light Fields[J]. Applied Optics, 2002, 41(6):1035-1050.
Cox W. Simlation, Modeling and Design of Underwater Optical Communication System[D]. North Carolina, US:North Carolina State University, 2012.
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