The energy levels of a rotating vibrator are calculated in considerable detail by means of the Wentzel-Brillouin-Kramers method. The new terms determined are ωₑz and a set of correction terms which appear in the earlier members of the equation. These correction terms enter in such a way that ωₑ is not exactly the coefficient of (v+1/2); Bₑ is not exactly the coefficient of $K(K+1)$, etc. However the differences are small and are detectable only in the case of light molecules. The correction terms are of the magnitude of Bₑ²ωₑ². Formulas for the effect of the correction terms on isotope shifts are given, and for the calculation of the correction terms themselves. Also a method is given for obtaining actual potential functions from band spectrum data, based on Morse's potential function. Finally the numerical magnitude of the correction terms for several states of H₂ and for NaH is discussed.
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J. L. Dunham (1932) studied this question.
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