Ab initio potential-energy surface for the He(S-1) plus NO(X (2)Pi) interaction and bound rovibrational states

Citation
J. Klos et al., Ab initio potential-energy surface for the He(S-1) plus NO(X (2)Pi) interaction and bound rovibrational states, J CHEM PHYS, 112(5), 2000, pp. 2195-2203
Citations number
32
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF CHEMICAL PHYSICS
ISSN journal
00219606 → ACNP
Volume
112
Issue
5
Year of publication
2000
Pages
2195 - 2203
Database
ISI
SICI code
0021-9606(20000201)112:5<2195:AIPSFT>2.0.ZU;2-0
Abstract
Adiabatic potential-energy surfaces for the (2)A' and (2)A " states of the He(S-1)-NO(X (2)Pi) complex have been calculated at the restricted coupled cluster level of theory including single, double, and noniterated triple ex citations [RCCSD(T)]. The potential-energy surface (PES) of the A' state ha s three minima: for the T-shaped geometry, barely skewed toward oxygen (R=6 .07 a(0), Theta=96.7 degrees, and D(e)approximate to 29.2 cm(-1)), and for two collinear forms. In contrast, PES of the A " state has two minima, both related to T-shaped forms: (i) A global minimum, with He shifted toward ni trogen (R=6.27 a(0), Theta=76.1 degrees, and D(e)approximate to 25.3 cm(-1) ), and a shoulderlike minimum, with He shifted toward oxygen (R=6.34 a(0), Theta=117.6 degrees, and D(e)approximate to 24.5 cm(-1)). The collinear for ms of the A " state correspond to saddle points. The A' surface lies above the A " surface, except in the vicinity of perpendicular arrangement. The i nteraction energies have been analyzed via perturbation theory of intermole cular forces. The shape and location of the minima is determined primarily by the anisotropy of the exchange component, and stronger repulsion of A' i s due to repulsion between the singly occupied anti-bonding pi* orbital and He. A variational calculation of the bound rovibrational states supported by the potential suggests that the HeNO complex is bound by about 7 cm(-1). The bound levels correlate with NO rotational levels with j=1/2 and j=3/2, and are well described as nearly free-rotor states in which j (NO rotation ) and L (end-over-end rotation of R) are nearly good quantum numbers. Excit ed intermolecular stretching vibrations are not predicted to be bound. (C) 2000 American Institute of Physics. [S0021-9606(00)30404-4].