Abstract

We derived a general formula of Franck–Condon integral for two-dimensional harmonic oscillators ( 〈 v 1 v 2 | v 1 ′ v 2 ′ 〉 ) taking into account the Duschinsky effect and applied it to study the photoelectron spectroscopy of SO 2 and SO 2 - . The equilibrium geometries and harmonic vibrational frequencies of SO 2 + , SO 2 and SO 2 - were calculated by using the density functional theory (B3LYP functional) and the coupled cluster singles and doubles with perturbative triples [CCSD(T)] methods with various basis sets up to 6-311+G(3df) and aug-cc-pVTZ. The adiabatic ionization energy and electron affinity were computed by using the CCSD(T) method extrapolated to the complete basis set limit with aug-cc-pVXZ (X = D, T, Q, 5). The simulated photoelectron spectra of both SO 2 and SO 2 - are in accord with the experiment. While the Duschinsky effect plays a role for some weak transitions of SO 2, it can be neglected for SO 2 - . A splitting observed in the experimental photoelectron spectrum of SO 2 is interpreted as contributing from hot bands and combination bands of ν 1 and ν 2, rather than arising from perturbation of a potential barrier as previous researchers proposed. The calculated adiabatic ionization energy and electron affinity are in agreement with the experiment within 0.027 and 0.040 eV, respectively.

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