TRANSITION AMPLITUDES OF SPHERICAL TOP MOLECULES FROM 0(3) $\times 0(3)$

Loading...
Thumbnail Image

Date

1976

Journal Title

Journal ISSN

Volume Title

Publisher

Ohio State University

Research Projects

Organizational Units

Journal Issue

Abstract

The rotational wave functions v(JKM) and the direction cosines (or D(1 K M)) can be seen as tensors of two 0(3) groups: the first, (m)0(3),describes transformations in the molecule fixed frame and the second, (F)0(3) in the space fixed frame. For a spherical top molecule, the groops of degeneracy of rotational and rovibrational energies are $(m){0}(3)\times(F){0}(3)$ reapectiely $(G = T_{d}$ for $XY_{4}$, $G = 0_{h}$ for $XY_{6}$). Energy levels are generally studied with the help of the reduced chain $G [FIGURE] \subset^{(m)} 0(3)$, but $G \times (F)^{0}(2)[FIGURE] \subset ^{(m)}0(3) \times ^{(F)}0(3)$ seems more appropriate for the calculation of transition amplitudes In this scheme, the states are labelled by |J$\ell$Rp; JM where J,$\ell$,R stand for the total, vibrational and rotational angular moments respectively; p and M are cubic and magnetic quantum numbers. Any transition Operator can be written in the form: $$^{(F)}A^{(X,L)}_{A_{1}M}= (D^{(L,L)} X^{(m)} A^{(\ell,0)} ){}^{(X,L)}_{A_{1}M}$$ where $D^{(L,L)}$ are products of direction cosines. Its matrix element is given by Wigner-Eckart theorem in $^{(m)} 0(3) x ^{(F)} 0(3)$: \begin{eqnarray*} &&(J^{\prime\prime} \ell^{\prime\prime} R^{\prime\prime} P^{\prime\prime} ; J^{\prime\prime} M^{\prime\prime} | ^{(F)} A^{(X , L)}_{A_{1}M } | J^{\prime} \ell^{\prime} R^{\prime} P^{\prime} ; J^{\prime} M^{\prime} ) =\\ &&\quad (- 1)^{R^{\prime\prime}} F^{(X R^{\prime\prime} R^{\prime\prime})}_{A_{1}P^{\prime\prime} P^{\prime}} (- 1)^{J^{\prime\prime} -M^{\prime\prime}} ({}^ {J^{\prime\prime} J^{\prime} L}_{-M^{\prime\prime} M^{\prime} M}) (J^{\prime\prime} \ell^{\prime} R^{\prime\prime} ; J^{\prime\prime} | {}^{(F)}A^{(X,L)}| J^{\prime} \ell^{\prime} R^{\prime} ; J^{\prime} )\end{eqnarray*} using cubic and standard 3j-symbols. Applications are given for Infrared, microwave, and Raman spectra.

Description

Author Institution: Laboratoire de Spectronomie Mol\'{e}culaire, Universite de Dijon

Keywords

Citation