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The magnetic hyperfine splitting of the ²S ground state of the lithium atom is calculated. It is shown that the discrepancy between experiment and the value calculated in the traditional Hartree-Fock approximation can be accounted for quantitatively by the exchange polarization effect, which distorts one $1s$ orbital relative to the other. The present calculation obtains a value within one percent of the experimental value. A general procedure is proposed for evaluating operators that do not commute with the Hamiltonian, when approximate variational methods must be used.
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R. K. Nesbet (1960) studied this question.
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