Orientation of O(3) and SU(2) ⊗ C1 representations in cubic point groups (Oh, Td) for application to molecular spectroscopy

被引:57
作者
Rey, M
Boudon, V
Wenger, C
Pierre, G
Sartakov, B
机构
[1] Univ Bourgogne, Phys Lab, CNRS, UMR 5027, F-21078 Dijon, France
[2] RAS, Inst Gen Phys, Moscow 119991, Russia
关键词
molecular spectroscopy; cubic tensors; orientation; high angular momentum values; half-integer angular momenta;
D O I
10.1016/S0022-2852(03)00056-0
中图分类号
O64 [物理化学(理论化学)、化学物理学]; O56 [分子物理学、原子物理学];
学科分类号
070203 ; 070304 ; 081704 ; 1406 ;
摘要
We propose a detailed method for the symmetrization of the standard O(3) or SU(2) circle times C-I basis \jtau, m> (tau = g or u) into the O-h or T-d point group. This is realized by means of an orientation matrix called G. The oriented basis obtained in this way allows matrix element calculations for rovibronic spectroscopic problems concerning octahedral or tetrahedral molecules. Particular attention has been put on careful phase choices. A numerical calculation of all the G matrix elements for both integer and half-integer j values up to 399/2 has been performed. Such high angular momentum values are necessary for the case of heavy molecules with high rotational excitation. To calculate the G coefficients with high precision at high j values we pre-calculated the necessary Wigner functions using symbolic MAPLE software and made then the numerical calculations with quadruple precision. The complete list of these coefficients can be obtained freely at the URL: http://www.u-bourgogne.fr/LPUB/group.html. As an illustration, we also present briefly an application to two typical spectroscopic calculations: the pure rotational levels of SF6 in its ground vibrational state and the nu(3) band of ReF6 (an open-shell molecule with an odd number of electrons and a fourfold degenerate electronic ground state). (C) 2003 Elsevier Science (USA). All rights reserved.
引用
收藏
页码:313 / 325
页数:13
相关论文
共 51 条
[1]   New accurate fit of an extended set of saturation data for the ν3 band of SF6:: Comparison of Hamiltonians in the spherical and cubic tensor formalisms [J].
Acef, O ;
Bordé, CJ ;
Clairon, A ;
Pierre, G ;
Sartakov, B .
JOURNAL OF MOLECULAR SPECTROSCOPY, 2000, 199 (02) :188-204
[2]  
Altmann S.A., 1986, Rotations, Quaternions and Double Groups
[3]   DOUBLE GROUPS AND PROJECTIVE REPRESENTATIONS .2. CLEBSCH-GORDON COEFFICIENTS [J].
ALTMANN, SL ;
PALACIO, F .
MOLECULAR PHYSICS, 1979, 38 (02) :513-526
[4]   DOUBLE GROUPS AND PROJECTIVE REPRESENTATIONS .1. GENERAL-THEORY [J].
ALTMANN, SL .
MOLECULAR PHYSICS, 1979, 38 (02) :489-511
[5]   DOUBLE GROUPS AND PROJECTIVE-REPRESENTATIONS .3. IMPROPER GROUPS [J].
ALTMANN, SL ;
HERZIG, P .
MOLECULAR PHYSICS, 1982, 45 (03) :585-604
[6]  
[Anonymous], 1982, Molecular vibrational-rotational spectra
[7]  
[Anonymous], 1992, Spherical Top Spectra
[8]  
Bethe H, 1929, ANN PHYS-BERLIN, V3, P133
[9]  
BIEDENHARN LC, 1981, ENCY MATH, V8
[10]   Spectroscopy of hexafluorides with an odd number of electrons: The vibronic bands of IrF6 [J].
Boudon, V ;
Rotger, M ;
Avignant, D .
JOURNAL OF MOLECULAR SPECTROSCOPY, 1996, 175 (02) :327-339