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探测距离达9.3个衰减长度的水下鬼成像。

Underwater ghost imaging with detection distance up to 9.3 attenuation lengths.

作者信息

Li Yuliang, Chen Mingliang, Qi Jinquan, Deng Chenjin, Du Longkun, Bo Zunwang, Han Chang, Mao Zhihua, He Yan, Shao Xuehui, Han Shensheng

出版信息

Opt Express. 2023 Nov 6;31(23):38457-38474. doi: 10.1364/OE.499186.

Abstract

Underwater ghost imaging LiDAR is an effective method of underwater detection. In this research, theoretical and experimental investigations were conducted on underwater ghost imaging, combining the underwater optical field transmission model with the inherent optical parameters of a water body. In addition, the Wells model and the approximate Sahu-Shanmugam scattering phase function were used to create a model for underwater optical transmission. The second-order Glauber function of the optical field was then employed to analyze the scattering field degradation during the transmission process. The simulation and experimental results verified that the proposed underwater model could better reveal the degrading effect of a water body on ghost imaging. A further series of experiments comparing underwater ghost imaging at different detection distances was also conducted. In the experimental system, gated photomultiplier tube (PMT) was used to filter out the peak of backscattering, allowing a larger gain to be set for longer-range detection of the target. The laser with a central wavelength of 532 nm was operated at a frequency of 2 KHz, with a single pulse energy of 2 mJ, a pulse width of 10 ns. High-reflective targets were imaged up to 65.2 m (9.3 attenuation lengths (ALs), attenuation coefficient c = 0.1426 m, and scattering coefficient b = 0.052 m) and diffuse-reflection targets up to 41.2 m (6.4 ALs, c = 0.1569 m, and b = 0.081 m). For the Jerlov-I (c = 0.048 m and b = 0.002 m) water body, the experimentally obtained maximum detection distance of 9.3 ALs can be equivalent to 193.7 m under the same optical system conditions.

摘要

水下鬼成像激光雷达是一种有效的水下探测方法。在本研究中,结合水体的水下光场传输模型和固有光学参数,对水下鬼成像进行了理论和实验研究。此外,使用韦尔斯模型和近似的萨胡 - 山穆加姆散射相位函数建立了水下光传输模型。然后利用光场的二阶格劳伯函数分析传输过程中的散射场退化。仿真和实验结果验证了所提出的水下模型能够更好地揭示水体对鬼成像的退化作用。还进行了一系列比较不同探测距离下水下鬼成像的实验。在实验系统中,使用门控光电倍增管(PMT)滤除后向散射峰值,从而可以为目标的远程探测设置更大的增益。中心波长为532 nm的激光器以2 KHz的频率运行,单脉冲能量为2 mJ,脉冲宽度为10 ns。高反射目标成像距离可达65.2 m(9.3个衰减长度(ALs),衰减系数c = 0.1426 m,散射系数b = 0.052 m),漫反射目标成像距离可达41.2 m(6.4个ALs,c = 0.1569 m,b = 0.081 m)。对于杰洛夫 - I型水体(c = 0.048 m,b = 0.002 m),在相同光学系统条件下,实验获得的9.3个ALs的最大探测距离相当于193.7 m。

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