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The vertical spectrum of H2CO revisited: (SC)2-CI and CC calculations
Authors:JOSE PITARCH-RUIZ  JOSE SANCHEZ-MARIN  ALFREDO SANCHEZ DE MERAS  DANIEL MAYNAU
Institution:1. Departament de Quimica-Fisica , Institut de Ciencia Molecular, Facultat de Ciencies Quimiques, Universitat de Valencia , Dr. Moliner 50, E-46100 , Burjassot (Valencia) , Spain;2. Laboratoire de Physique Quantique, URA 505 , Université Paul Sabatier , 118 route de Narbonne, 31062 , Toulouse Cedex , France
Abstract:The vertical electronic spectrum of formaldehyde has been studied by means of (SC)2-MR-SDCI and CCLR methods. Two basis sets of atomic natural orbitals (ANOs) complemented with a one-centre series of Rydberg orbitals were used. The first was taken from the CASPT2 study by Merchán, M., and Roos, B. O., 1995, Theoret. Chim. Acta, 92, 221, and may be described as C,O4s3pld]/H2slp] with a lslpld Rydberg series centred in the charge centroid of the 2B2 state of the cation. The second was a larger basis set that may be described as C,O6s5p3d2f]/H4s3p2d] + 3s3p3d in the same centre. The (SC)2 dressing may be applied efficiently to an MR-SDCI method and comparison with the dressed CAS-SDCI is satisfactory, in spite of the remarkable reduction in the CI space dimension. The consistency of the (SC)2-MR-SDCI results was tested also against the CCLR and CASPT2 results using the same basis sets and against the CCLR results using Dunning's aug- and daug-cc-pVQZ basis sets. The 3A1(π → π *) state is correctly placed as the second excited triplet while the highly multi-configurational nature of the 1A1(π → π *) state is confirmed as well as its greatly mixed valence-Rydberg nature. This state is predicted as lying under the 10 eV level, on top of the (ny → 3d) Rydberg states that are predicted in the 8.9–9.5eV region. The 5 1B2(ny → 4s) Rydberg state and the 1B2y → π*) also are predicted in this region. The triplet states also were calculated with the (SC)2-MR-SDCI method. The vertical ordering of the 2 1A1(ny → 3py) and 2 1B2(ny → 3pz) states is discussed, as well as that of the 1B1(σ → π*) and the Rydberg 1B1(ny → 3dxy) states. This work shows the highly reliable values that may be reached applying the dressing method along with a large basis set. Such a procedure is made possible using an MR-SDCI selection of spaces instead of the CAS-SDCI that was used up to now in most (SC)2 dressing applications.
Keywords:symmetric-top molecules  variational calculation  irreducible tensor  finite basis representation  vibration energy levels
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