Abstract
In a previous paper [J. Math. Phys. 15, 1901 (1975)] we derived an equation governing the mutual coherence function, {Γ̂}, of an initial plane wave signal propagating in an anisotropic random medium. In Eq. (49) of that paper we made a strong narrow‐angle approximation which allowed us to derive an ordinary differential equation for {Γ̂}. Here we derive an integro–differential equation for {Γ̂} in which this approximation is not made. We show that for the horizontal scattering cases considered in the previous paper the approximation is valid. The vertical spectrum, however, is changed somewhat.

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