Abstract
Mathematical formalism of the Low Rank Perturbation method (LRP) is applied to the vibrational isotope effect in the harmonic approximation with a standard assumption that force field does not change under isotopic substitutions. A pair of two n-atom isotopic molecules A and B which are identical except for isotopic substitutions at ρ atomic sites is considered. In the LRP approach vibrational frequencies ωk and normal modes \({\left|{\Psi_k}\right\rangle}\) of the isotopomer B are expressed in terms of the vibrational frequencies νi and normal modes \({\left|{\Phi_i}\right\rangle}\) of the parent molecule A. In those relations complete specification of the normal modes \({\left|{\Phi_i}\right\rangle}\) is not required. Only amplitudes \({\left\langle{\tau s}|{\Phi_i}\right\rangle}\) at sites τ affected by the isotopic substitutions and in the coordinate direction s (s = x, y, z) are needed. Out-of-plane vibrations of the (H,D)-benzene isotopomers are considered. Standard error of the LRP frequencies with respect to the DFT frequencies is on average \({\Delta \approx 0.48\,{\rm cm}^{-1}}\) . This error is due to the uncertainty of the input data (± 0.5 cm−1) and in the absence of those uncertainties and in the harmonic approximation it should disappear. In comparing with experiment, one finds that LRP frequencies reproduces experimental frequencies of (H,D)-benzene isotopomers better (\({\Delta_{LRP}\approx 4.74\,{\rm cm}^{-1}}\)) than scaled DFT frequencies (\({\Delta_{DFT}\approx 6.79\,{\rm cm}^{-1}}\)) which are designed to minimize (by frequency scaling technique) this error. In addition, LRP is conceptually and numerically simple and it also provides a new insight in the vibrational isotope effect in the harmonic approximation.
Published Version
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