The frequency‐dependent dipole polarizability, α(E), is calculated using the second‐order polarization propagator approximation (SOPPA). We have shown how to express α(E) as a function of E2 and thus obtained a form of α(E) that can be used to compute C6‐coefficients without invoking complex arithmetic. For He we find that SOPPA recovers a large fraction of the correlation contribution for all frequencies, whereas for H2 where the correlation contributions are much smaller and also basis set‐dependent, we find a less definite trend of SOPPA relative to RPA.
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Sauer et al. (1991) studied this question.
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