Abstract

In the present work systematic procedures for the balanced description of the lowest singlet excited valence and Rydberg states of butadiene, especially for the correct description of the 11B u state, are presented. In the first step of the calculation averaged natural orbitals (ANOs) were computed from the density matrices of the ground state, the 21A g and the 11B u states. For the 11B u state the configuration interaction (CI) wave function used for the computation of the respective density matrix contained all possible single and double excitations from the 1b g (π) orbital into all virtual orbitals and double excitations describing σ–π electron correlation. For the ground and 21A g states a standard multireference (MR) CI with singles and doubles (CISD)/complete-active-space (CAS)(4,4) wave function was used. In the second step, these ANOs were used in extended MR-CISD, MR-CISD with Davidson correction and MR averaged quadratic coupled cluster calculations. This scheme was also extended to state-averaging including the four lowest Rydberg states 11B g (3s), 11A u (3p σ ), 21A u (3p σ ) and 21B u (3p π). Our best value for the vertical excitation energy to the 11B u state is 6.18 eV, close to previous equation-of-motion coupled-cluster with singles and doubles including noniterative triples [EOM - CCSD( )] and complete-active-space perturbation theory to second order (CASPT2) results, but significantly lower than most of the previous MR-CI and MR-CI based results. The computed vertical excitation energy to the 21A g state of 6.55 eV is significantly below previous EOM-CCSD(T) and EOM - CCSD( ) results and demonstrates the deficiencies of these methods in the case of MR situations. On the other hand, this excitation energy is larger than previous CASPT2 results for the 21A g state. The character of the 11B u state is predominantly of valence character, but is more diffuse than the ground state. <x 2>values for the 11B u state range between 25.4 and 26.3a 0 2 in the three-state calculations.

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