The vertical spectrum of H2CO revisited:: (SC)2-CI and CC calculations

被引:16
作者
Pitarch-Ruiz, J
Sanchez-Marin, J
De Meras, AS
Maynau, D
机构
[1] Univ Valencia, Fac Ciencias Quim, Dept Quim Fis, Inst Ciencias Mol, E-46100 Burjassot, Spain
[2] Univ Toulouse 3, Phys Quant Lab, URA 505, F-31062 Toulouse, France
关键词
D O I
10.1080/0026897021000034503
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
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 Merchan, M., and Roos, B.O., 1995, Theoret. Chim. Acta, 92, 227, and may be described as C,O[4s3p1d]/H[2s1p] with a 1s1p1d Rydberg series centred in the charge centroid of the B-2(2) state of the cation. The second was a larger basis set that may be described as C,O[6s5p3d2f]/H[4s3p2d]+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 Cl 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 (3)A(1) (pi-->pi*) state is correctly placed as the second excited triplet while the highly multi-configurational nature of the (1)A(1) (pi-->pi*) 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 (n(y)-->3d) Rydberg states that are predicted in the 8.9-9.5 eV region. The 5 B-1(2) (n(y)-->4s) Rydberg state and the B-1(2)(sigma(y)-->pi*) 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 (1)A(1) (n(y)-->3p(y)) and 2 B-1(2)(n(y)-->3p(z)) states is discussed, as well as that of the B-1(1)(sigma-->pi*) and the Rydberg B-1(1)(n(y)-->3d(xy)) 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.
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页码:483 / 494
页数:12
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