Ab initio characterization of the structure and energetics of the ArHF complex

被引:56
作者
vanMourik, T
Dunning, TH
机构
[1] Environ. Molec. Sciences Laboratory, Richland
关键词
D O I
10.1063/1.475148
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 ArHF complex has been investigated using correlation consistent basis sets at several levels of theory, including Moller-Plesset perturbation theory (MP2, MP3, MP4) and coupled cluster techniques [CCSD, CCSD(T)]. The three stationary points (the primary linear Ar-HF minimum, the secondary linear Ar-FH minimum, and the interposed transition state TS) on the counterpoise-corrected potential energy surface have been characterized. Calculations with the aug-cc-pV5Z basis set predict D-e for the Ar-HF minimum to be (with estimated complete basis set limits in parentheses) -215 (-218) cm(-1) for MP3 and -206 (-211) cm(-1) for CCSD(T). For the Ar-FH minimum and the TS, calculations with the d-aug-cc-pVQZ sets predict D-e's (and CBS limits) of -97 (-99) and -76 (-78) cm(-1) (MP4) and -93 (-94) and -75 (-76) cm(-1) [CCSD(T)], respectively. The corresponding values for the H6(4,3,2) potential of Hutson [J. Chem. Phys. 96, 6752 (1992)] are -211.1 +/- 4 cm(-1), -108.8 +/- 10 cm(-1), and -82.6 +/- 10 cm(-1). While the agreement of our CCSD(T) estimate with Hutson's value is excellent for the global minimum, it is less so for the other two stationary points, suggesting that the H6(4,3,2) potential may be too attractive around the secondary minimum and the transition state. (C) 1997 American Institute of Physics.
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页码:2451 / 2462
页数:12
相关论文
共 63 条
[1]   ENERGY-TRANSFER AS A FUNCTION OF COLLISION ENERGY .4. STATE-TO-STATE CROSS-SECTIONS FOR ROTATIONAL-TO-TRANSLATIONAL ENERGY-TRANSFER IN HF+NE, AR, AND KR [J].
BARNES, JA ;
KEIL, M ;
KUTINA, RE ;
POLANYI, JC .
JOURNAL OF CHEMICAL PHYSICS, 1982, 76 (02) :913-930
[2]  
BOYS SF, 1970, MOL PHYS, V19, P53
[3]   OBSERVATION OF ARHF(3000) AND ITS COMBINATION-MODES BY LASER-INDUCED FLUORESCENCE [J].
CHANG, HC ;
KLEMPERER, W .
JOURNAL OF CHEMICAL PHYSICS, 1993, 98 (04) :2497-2506
[4]   THE AR-HF INTERMOLECULAR POTENTIAL - OVERTONE SPECTROSCOPY AND AB-INITIO CALCULATIONS [J].
CHANG, HC ;
TAO, FM ;
KLEMPERER, W ;
HEALEY, C ;
HUTSON, JM .
JOURNAL OF CHEMICAL PHYSICS, 1993, 99 (12) :9337-9349
[5]  
DEEGAN MJO, 1992, UNPUB IMPLEMENTATION
[6]   THE ROTATIONAL AND HYPERFINE SPECTRUM OF AR-HF [J].
DIXON, TA ;
JOYNER, CH ;
BAIOCCHI, FA ;
KLEMPERER, W .
JOURNAL OF CHEMICAL PHYSICS, 1981, 74 (12) :6539-6543
[7]   The Wentzel-Brillouin-Kramers method of solving the wave equation [J].
Dunham, JL .
PHYSICAL REVIEW, 1932, 41 (06) :713-720
[9]   OBSERVATION OF 3 INTERMOLECULAR VIBRATIONAL-STATES OF AR-HF [J].
DVORAK, MA ;
REEVE, SW ;
BURNS, WA ;
GRUSHOW, A ;
LEOPOLD, KR .
CHEMICAL PHYSICS LETTERS, 1991, 185 (3-4) :399-402
[10]   HIGH-RESOLUTION INFRARED OVERTONE SPECTROSCOPY OF ARHF VIA NDYAG/DYE LASER DIFFERENCE-FREQUENCY-GENERATION [J].
FARRELL, JT ;
SNEH, O ;
MCILROY, A ;
KNIGHT, AEW ;
NESBITT, DJ .
JOURNAL OF CHEMICAL PHYSICS, 1992, 97 (11) :7967-7978