Abstract

Electric-field-controlled two-dimensional Raman–Nath diffraction has been realized using a photorefractive diffraction grating. The grating was produced by two-wave coupling (at a wavelength of 632.8 nm) at small incidence angles using a potassium lithium tantalate niobate single crystal. Results for the Raman–Nath diffraction from the g 44 grating are presented, in which the externally applied field is perpendicular to both the grating vector and the wave vector of the incident beam. Two pairs of coherent beams were used to record the grating for two-dimensional Raman–Nath diffraction. The wave vector and the polarization of one pair lay in the ( x, z) plane, and those of the other pair lay in the ( y, z) plane. The influence of the applied electric field was studied, and the results show that the intensity of the Raman–Nath diffraction could be controlled by the direction and intensity of the applied field.

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