Zero field splitting of the chalcogen diatomics using relativistic correlated wave-function methods

J. B. Rota, S. Knecht, T. Fleig, D. Ganyushin, T. Saue, F. Neese, H. Bolvin

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Abstract

The spectrum arising from the ()2 configuration of the chalcogen dimers, namely, the X21, a2, and b0 states, is calculated using wave-function theory based methods. Two-component (2c) and four-component (4c) multireference configuration interaction (MRCI) and Fock-space coupled cluster (FSCC) methods are used as well as two-step methods spin-orbit complete active space perturbation theory at 2nd order (SO-CASPT2) and spin-orbit difference dedicated configuration interaction (SO-DDCI). The energy of the X21 state corresponds to the zero-field splitting of the ground state spin triplet. It is described with high accuracy by the 2-and 4-component methods in comparison with experiment, whereas the two-step methods give about 80 of the experimental values. The b0 state is well described by 4c-MRCI, SO-CASPT2, and SO-DDCI, but FSCC fails to describe this state and an intermediate Hamiltonian FSCC ansatz is required. The results are readily rationalized by a two-parameter model; , the spinor splitting by spin-orbit coupling and K, the exchange integral between the 1* and the-1* spinors with, respectively, angular momenta 1 and-1. This model holds for all systems under study with the exception of Po2.

Original languageEnglish
Article number114106
JournalJournal of Chemical Physics
Volume135
Issue number11
DOIs
StatePublished - Sep 21 2011
Externally publishedYes

Funding

This work has been supported by the ANR-09-BLAN-0195 TEMAMA. S.K. gratefully acknowledges postdoctoral research grants from l’Université de Strasbourg (UdS) and the Natural Science Foundation (FNU) of the Danish Agency for Science, Technology, and Innovation. This work has been supported through ample computing time at the supercomputer centers of UdS and the Danish Center for Scientific Computing at SDU Odense. F.N. and D.G. gratefully acknowledge financial support of this work by the University of Bonn, the Max Planck Institut, and the SFB 813 (“Chemistry at spin centers”). The authors would like to acknowledge interesting and most helpful remarks of the referees.

FundersFunder number
ANR-09-BLAN-0195 TEMAMA
Danish Agency for Science, Technology, and Innovation
Natural Science Foundation
Shandong University
Rheinische Friedrich-Wilhelms-Universität Bonn
Fujian Normal University
Max Planck Institute for Nuclear PhysicsSFB 813
l’Université de Strasbourg

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