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Numerical Modelling of Fluorescence Lidar Signals in Case 1 Marine Waterrs L&E, Vol.33, No.5, 2025

Light & Engineering 33 (5) 2025

Volume 33
Date of publication 10/20/2025
Pages 89–96

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Numerical Modelling of Fluorescence Lidar Signals in Case 1 Marine Waterrs L&E, Vol.33, No.5, 2025
Articles authors:
Dmitry I. Glukhovets, Yuri A. Goldin, Sergey V. Sheberstov, Lev E. Yakushkin

Dmitry I. Glukhovets, Ph. D. in Physical and Mathematical Sciences. He graduated in 2016 from the Faculty of Radio Engineering and Cybernetics of MIPT. At present, he is a head of the Ocean Optics Laboratory of the Oceanology Institute at the Russian Academy of Sciences

Yuri A. Goldin, Ph. D. in Physical and Mathematical Sciences. He graduated from the Physics Department of Moscow State University in 1965. He was the leading researcher at the Institute of Oceanology at the Russian Academy of Sciences.

Sergey V. Sheberstov graduated from the Faculty of Mechanics and Mathematics of Moscow State University in 1967. He is the senior researcher at the Institute of Oceanology at the Russian Academy of Sciences

Lev E. Yakushkin graduated from the Physics Department of Moscow State University in 2022. At present, he is the engineer at the Institute of Oceanology of the Russian Academy of Sciences, postgraduate student at Moscow State University

Abstract:
Numerical Monte Carlo modelling of integrated fluorescence lidar returns in Case 1 marine waters was conducted. A dedicated program implementing coordinate recording of individual inelastic scattering events was developed to address these objectives. Modelled Raman scattering spectra and chlorophyll fluorescence intensities were obtained for three pigment concentrations and two probing wavelengths: 355 nm and 532 nm. Contributions to the integrated return signal from photons originating at different water depths and radial distances from the beam axis were quantified. For the first time, the spatial dimensions of the inelastic scattering signal formation volume were estimated. Results demonstrate that the signal is predominantly contributed by the region concentrated along the probing laser beam axis.
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