The direct observation of polarization mixing in nuclear Bragg scattering of synchrotron radiation by {α}-⁵⁷Fe''₂{O}₃$ is reported. Application of a magnetic bias field having the appropriate orientation was shown to produce almost complete rotation of the {σ}-polarized incident beam to a {π}-polarized diffracted beam. Rotation of this field about the diffraction vector through 90^∘{} caused the diffracted beam polarization to change continuously from {σ} through elliptical to {π}, as predicted theoretically.
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Siddons et al. (1989) studied this question.
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