A solution of the wave equation for the nuclear motion of a diatomic molecule with a Morse potential function and the rotational term included is given. The wave functions are found to have the same form as the functions obtained when the rotational term is neglected. The constants Dₑ and αₑ in the equations Bᵥ=Bₑ-αₑ(v+1/2), Dᵥ=Dₑ+βₑ(v+1/2), are found to be given by the relations Dₑ=-4Bₑ³ωₑ² αₑ=2xₑBₑ(3[Bₑxₑωₑ]1/2-3Bₑxₑωₑ), a result which can also be derived from Dunham's formulas. Eq. (2) differs from the corresponding relation in Kratzer's formula by the term in parenthesis. This term is fairly constant for a number of molecules and has an average value of 0.7±{}0.1 as was found empirically by Birge. The values of αₑ given by (2) show satisfactory agreement with experimental values for many molecules.
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C. L. Pekeris (1934) studied this question.
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