Rotational transitions in the collisions of diatomic molecules are treated by means of a rigid body approximation. The deviation from sphericity is assumed to be sufficiently small that it may be treated as a perturbation. The differential cross section is calculated for the H2-HD collision in which the hydrogen remains in its ground state while the hydrogen deuteride goes from its ground state to the first excited rotational state.
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Gioumousis et al. (1962) studied this question.
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