1988
DOI: 10.1364/ao.27.002111
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Intensity images and statistics from numerical simulation of wave propagation in 3-D random media

Abstract: An extended random medium is modeled by a set of 2-D thin Gaussian phase-changing screens with phase power spectral densities appropriate to the natural medium being modeled. Details of the algorithm and limitations on its application to experimental conditions are discussed, concentrating on power-law spectra describing refractive-index fluctuations of the neutral atmosphere. Inner and outer scale effects on intensity scintillation spectra and intensity variance are also included. Images of single realization… Show more

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Cited by 415 publications
(206 citation statements)
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“…(17). For a real-valued, asymmetric phase functionξ * (K) = ξ(−K), however, in the numerical simulation one normally uses a completely asymmetric two-dimensional random complex functionξ(K), which implies that the resulting phase function is complex [28,29] …”
Section: Theoretical Backgroundmentioning
confidence: 99%
See 1 more Smart Citation
“…(17). For a real-valued, asymmetric phase functionξ * (K) = ξ(−K), however, in the numerical simulation one normally uses a completely asymmetric two-dimensional random complex functionξ(K), which implies that the resulting phase function is complex [28,29] …”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…These N runs are used to perform ensemble averaging for each of the elements in the evolution sequence, as expressed in Eq. (28), to obtain a sequence of density matrices that represent the evolution of the bi-photon state from an initial pure state to the mixed quantum state that one would observe at a particular point along the propagation path.…”
Section: Numerical Simulation Proceduresmentioning
confidence: 99%
“…In order to interpret the observed C / N 0 fluctuations we performed a series of MPS simulations (Knepp, 1983;Martin and Flatté, 1988;Grimault, 1998). The propagation of a plane wave through the lower troposphere is modelled by a series of 500 non-equidistant phase screens covering the range from the receiver to a distance of 500 km.…”
Section: Simulationsmentioning
confidence: 99%
“…For more general conditions (strong scintillations), the moment equations are so difficult that they are solved only for some special cases and approximations. A variety of techniques have been proposed such as the parabolic equation method [16,59], extended Huygens-Fresnel principle [16,60], multiple phase screen [61], the path integral [62,63] and numerical techniques [64,65]. Among these, the parabolic equation method with the Markov approximation [59,66] occupies an important place.…”
Section: Theory Of Scintillationmentioning
confidence: 99%