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Zero field splitting of the chalcogen diatomics using relativistic correlated wave-function methods
Author(s) -
J.-B. Rota,
Stefan Knecht,
Timo Fleig,
Dmitry Ganyushin,
Trond Saue,
Frank Neese,
Hélène Bolvin
Publication year - 2011
Publication title -
the journal of chemical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.071
H-Index - 357
eISSN - 1089-7690
pISSN - 0021-9606
DOI - 10.1063/1.3636084
Subject(s) - complete active space , coupled cluster , wave function , ansatz , hamiltonian (control theory) , spinor , multireference configuration interaction , diatomic molecule , configuration interaction , chemistry , ground state , fock space , atomic physics , physics , zero field splitting , quantum mechanics , mathematics , density functional theory , molecule , excited state , spin polarization , mathematical optimization , electron , basis set
International audienceThe spectrum arising from the (π*)(2) configuration of the chalcogen dimers, namely, the X(2)1, 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 X(2)1 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; Δε, the π* spinor splitting by spin-orbit coupling and K, the exchange integral between the π(1)* and the π(-1)* spinors with, respectively, angular momenta 1 and -1. This model holds for all systems under study with the exception of Po(2)

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