Abstract
The steady-state two-dimensional coupled wave equations describing the photorefractive double phase conjugate mirror with TE-polarized pumps, and which are derived directly from Maxwell's equations without employing the slowly varying envelope approximation (SVEA), are solved analytically in the undepleted pumps approximation for equal pump intensities and angles of incidence. The solutions are compared with those obtained using the SVEA, and the predictions of each approach with regard to the operation of the double phase conjugate mirror are discussed.
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