4.2 Article

The V state of ethylene: valence bond theory takes up the challenge

Journal

THEORETICAL CHEMISTRY ACCOUNTS
Volume 133, Issue 3, Pages -

Publisher

SPRINGER
DOI: 10.1007/s00214-013-1441-x

Keywords

Valence bond; Quantum Monte Carlo; V state of ethylene; Breathing orbitals

Funding

  1. Natural Science Foundation of China [21120102035, 21273176, 21290193]
  2. Israel Science Foundation (ISF) [1183/13]

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The ground state and first singlet excited state of ethylene, so-called N and V states, respectively, are studied by means of modern valence bond methods. It is found that extremely compact wave functions, made of three VB structures for the N state and four structures for the V state, provide an N -> V transition energy of 8.01 eV, in good agreement with experiment (7.88 eV for the N -> V transition energy estimated from experiments). Further improvement to 7.96/7.93 eV is achieved at the variational and diffusion Monte Carlo (MC) levels, respectively, VMC/DMC, using a Jastrow factor coupled with the same compact VB wave function. Furthermore, the measure of the spatial extension of the V state wave function, 19.14 a (0) (2) , is in the range of accepted values obtained by large-scale state-of-the-art molecular orbital-based methods. The sigma response to the fluctuations of the pi electrons in the V state, known to be a crucial feature of the V state, is taken into account using the breathing orbital valence bond method, which allows the VB structures to have different sets of orbitals. Further valence bond calculations in a larger space of configurations, involving explicit participation of the sigma response, with 9 VB structures for the N state and 14 for the V state, confirm the results of the minimal structure set, yielding an N -> V transition energy of 7.97 eV and a spatial extension of 19.16 a (0) (2) for the V state. Both types of valence bond calculations show that the V state of ethylene is not fully ionic as usually assumed, but involving also a symmetry-adapted combination of VB structures each with asymmetric covalent pi bonds. The latter VB structures have cumulated weights of 18-26 % and stabilize the V state by about 0.9 eV. It is further shown that these latter VB structures, rather than the commonly considered zwitterionic ones, are the ones responsible for the spatial extension of the V state, known to be ca. 50 % larger than the V state.

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