The properties of Hartree–Fock wavefunctions are used to derive a number of new expressions for upper and lower bounds to the true expectation value of an arbitrary one-electron operator. These expressions depend on the prior knowledge of upper and lower bounds to the overlap between the Hartree–Fock and true wavefunctions. A new extrapolation method is presented to obtain accurate bounds to these overlaps. A critical study is made of the effectiveness and accuracy of these new error bounds as applied to the systems He, He2, LiH, and Be.
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Millard H. Alexander (1969) studied this question.
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