Abstract
The theory of two-magnon Raman scattering in an antiferromagnet, given by Elliott and Thorpe, (abstr. A15401 of 1970) is extended to the spin-flop phase. Application is made to the perovskite and K2NiF4 structures and the lineshape predicted. The main features are a broadening of the line and the appearance of additional structure, together with a decrease in intensity.
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