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Molecules diffracted from a crystal can exchange energy between translation and rotation. Such an interchange can lead to an extremum in the scattering angle as a function of the incident wavelength; this in turn concentrates scattered intensity at the extremal angle, causing a singularity in the differential cross section. Extremal scattering in rotationally inelastic collisions is explored quantitiatively for the diffraction of hydrogenic molecules and shown to affect significantly experiments with thermal beams.
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Rowe et al. (1975) studied this question.
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