2006
DOI: 10.1364/ao.45.003534
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Characterizing the propagation path in moderate to strong optical turbulence

Abstract: In February 2005 a joint atmospheric propagation experiment was conducted between the Australian Defence Science and Technology Organisation and the University of Central Florida. A Gaussian beam was propagated along a horizontal 1500 m path near the ground. Scintillation was measured simultaneously at three receivers of diameters 1, 5, and 13 mm. Scintillation theory combined with a numerical scheme was used to infer the structure constant C2n, the inner scale l0, and the outer scale L0 from the optical measu… Show more

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Cited by 31 publications
(14 citation statements)
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“…Optical measurements, in combination with a scintillation theory developed by Andrews et al 17,25 were used to infer the refractive index structure parameter C n 2 , the inner scale of turbulence l 0 , and the outer scale of turbulence L 0 , along the propagation path. 26 The theoretical expressions for the scintillation index, at a fixed range and wavelength, depend on four parameters: C n 2 , l 0 , L 0 , and D. By specifying three different collecting aperture sizes, and measuring the corresponding scintillation index experimentally, a minimization problem for the atmospheric parameters was created. It was solved numerically with the downhill simplex method, 26,27 which is a multidimensional minimization algorithm that requires only function evaluations, not derivatives.…”
Section: A Experimental Datamentioning
confidence: 99%
See 1 more Smart Citation
“…Optical measurements, in combination with a scintillation theory developed by Andrews et al 17,25 were used to infer the refractive index structure parameter C n 2 , the inner scale of turbulence l 0 , and the outer scale of turbulence L 0 , along the propagation path. 26 The theoretical expressions for the scintillation index, at a fixed range and wavelength, depend on four parameters: C n 2 , l 0 , L 0 , and D. By specifying three different collecting aperture sizes, and measuring the corresponding scintillation index experimentally, a minimization problem for the atmospheric parameters was created. It was solved numerically with the downhill simplex method, 26,27 which is a multidimensional minimization algorithm that requires only function evaluations, not derivatives.…”
Section: A Experimental Datamentioning
confidence: 99%
“…26 The theoretical expressions for the scintillation index, at a fixed range and wavelength, depend on four parameters: C n 2 , l 0 , L 0 , and D. By specifying three different collecting aperture sizes, and measuring the corresponding scintillation index experimentally, a minimization problem for the atmospheric parameters was created. It was solved numerically with the downhill simplex method, 26,27 which is a multidimensional minimization algorithm that requires only function evaluations, not derivatives. The experimental scintillation index was measured for the same 5 min of data used to calculate the PDF, at each receiving aperture (1, 5, and 13 mm diameter).…”
Section: A Experimental Datamentioning
confidence: 99%
“…Unlike previous work [4,17], an optical intensity-modulated sinusoid is transmitted through the channel to measure the loss and fading, h(t) in Eq. (2).…”
Section: A Measurement Proceduresmentioning
confidence: 99%
“…A number of recent papers [1][2][3][4][5][6][7][8][9][10][11][12][13][14] discussed the issues related to the performance of the Free-Space Optical Communication Systems (FSO) in the turbulent atmosphere. In the literature the emphasis is made on the mitigating the signal fading due to the turbulence-induced fluctuation by the aperture averaging of the scintillations or spatial diversity.…”
Section: Introductionmentioning
confidence: 99%