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A general theory of the magnetic hyperfine structure in diatomic molecules, including states other than ^1 states, is given. The magnetic hyperfine interaction is derived from the Dirac equation for the electron in the molecular potential field. First-order hyperfine structure formulas are given for the various vector coupling schemes characteristic of molecular states. The ^1 magnetic hyperfine structures are obtained from second order hyperfine interactions. Applications to the N^14O^16 and O^16O^17 microwave spectra are discussed.
Frosch et al. (Mon,) studied this question.
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