Issue 5, 1994

Configuration interaction studies on the S2 surface of H2CO: 21A′(σ, π*/π, π*) as perturber of 1 1B2(n, 3s)

Abstract

MRD-Cl calculations reveal that the third singlet surface S2 of H2CO exhibits two energetically close-lying minima. The more stable state at 7.09 eV is the experimentally known 1 1B2(n, 3s). The second minimum at 7.53 eV corresponds to the pyramidal state 2 1A′, of mixed σ, π* and π, π* character near equilibrium. This S2 valence minimum, which apparently has not been experimentally observed, is suggested to cause the blue shift of the S2â†� S0 system of H2CO in condensed media (as well as in related aldehydes and ketones), ruling out n →σ*co(1B2) as responsible for this blue shift. The 21A′, state is non-adiabatically coupled with the ground state, explaining the observed predissociation of 11B2 into the CH2+ O continuum. The planar (C2v) and pyramidal (Cs) minima can be connected only through a C1 intermediary, requiring participation of the antisymmetric CH-stretch and CH2 bend vibrations, besides the CO-stretch and out-of-plane modes. A dipole moment µ=+3.45 D (1D ≈ 3.335 64 × 10–30 C m) with polarity (H2C)O+ is predicted for 11B2(n, 3s) at equilibrium, at variance with an experimental µ of +0.33 D. An experimental route for studying the valence region of S2 is proposed.

Article information

Article type
Paper

J. Chem. Soc., Faraday Trans., 1994,90, 683-688

Configuration interaction studies on the S2 surface of H2CO: 21A′(σ, π*/π, π*) as perturber of 1 1B2(n, 3s)

M. Hachey, P. J. Bruna and F. Grein, J. Chem. Soc., Faraday Trans., 1994, 90, 683 DOI: 10.1039/FT9949000683

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