It is demonstrated, through terms of second order in the fluctuating part of the index of refraction, that the first and second statistical moment, as obtained from the Dyson and the Bethe-Salpeter equation, respectively, of an optical wave propagating in a random medium are identical to that obtained directly from the extended Huygens-Fresnel principle.
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H. T. Yura (1972) studied this question.
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