Accurate calculations on 9 螞-S and 28 惟 states of NSe radical in the gas phase: Potential energy curves, spectroscopic parameters and spin-orbit couplings
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文摘
The potential energy curves (PECs) of 28 惟 states generated from 9 螞-S states (X2螤, 14螤, 16螤, 12+, 14+, 16+, 14-, 24螤 and 14螖) are studied for the first time using an ab initio quantum chemical method. All the 9 螞-S states correlate to the first two dissociation limits, N(4Su) + Se(3Pg) and N(4Su) + Se(3Dg), of NSe radical. Of these 螞-S states, the 16+, 14+, 16螤, 24螤 and 14螖 are found to be rather weakly bound states. The 12+ is found to be unstable and has double wells. And the 16+, 14+, 14螤 and 16螤 are found to be the inverted ones with the SO coupling included. The PEC calculations are made by the complete active space self-consistent field method, which is followed by the internally contracted multireference configuration interaction approach with the Davidson modification. The spin-orbit coupling is accounted for by the state interaction approach with the Breit-Pauli Hamiltonian. The convergence of the present calculations is discussed with respect to the basis set and the level of theory. Core-valence correlation corrections are included with a cc-pCVTZ basis set. Scalar relativistic corrections are calculated by the third-order Douglas-Kroll Hamiltonian approximation at the level of a cc-pV5Z basis set. All the PECs are extrapolated to the complete basis set limit. The variation with internuclear separation of spin-orbit coupling constants is discussed in brief for some 螞-S states with one shallow well on each PEC. The spectroscopic parameters of 9 螞-S and 28 惟 states are determined by fitting the first ten vibrational levels whenever available, which are calculated by solving the rovibrational Schr枚dinger equation with Numerov鈥檚 method. The splitting energy in the X2螤 螞-S state is determined to be about 864.92 cm鈭?, which agrees favorably with the measurements of 891.80 cm鈭?. Moreover, other spectroscopic parameters of 螞-S and 惟 states involved here are also in fair agreement with available measurements. It demonstrates that the spectroscopic parameters reported here can be expected to be reliable predicted ones.

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