scholarly journals Transformation Properties under the Operations of the Molecular Symmetry Groups G36 and G36(EM) of Ethane H3CCH3

Symmetry ◽  
2019 ◽  
Vol 11 (7) ◽  
pp. 862
Author(s):  
Mellor ◽  
Yurchenko ◽  
Mant ◽  
Jensen

In the present work, we report a detailed description of the symmetry propertiesof the eight-atomic molecule ethane, with the aim of facilitating the variational calculations ofrotation-vibration spectra of ethane and related molecules. Ethane consists of two methyl groupsCH3 where the internal rotation (torsion) of one CH3 group relative to the other is of large amplitudeand involves tunnelling between multiple minima of the potential energy function. The molecularsymmetry group of ethane is the 36-element group G36, but the construction of symmetrised basisfunctions is most conveniently done in terms of the 72-element extended molecular symmetrygroup G36(EM). This group can subsequently be used in the construction of block-diagonal matrixrepresentations of the ro-vibrational Hamiltonian for ethane. The derived transformation matricesassociated with G36(EM) have been implemented in the variational nuclear motion program TROVE(Theoretical ROVibrational Energies). TROVE variational calculations are used as a practical exampleof a G36(EM) symmetry adaptation for large systems with a non-rigid, torsional degree of freedom.We present the derivation of irreducible transformation matrices for all 36 (72) operations of G36(M)(G36(EM)) and also describe algorithms for a numerical construction of these matrices based on aset of four (five) generators. The methodology presented is illustrated on the construction of thesymmetry-adapted representations both of the potential energy function of ethane and of the rotation,torsion and vibration basis set functions.

2004 ◽  
Vol 82 (6) ◽  
pp. 867-872 ◽  
Author(s):  
Emily J Gilles ◽  
Jaebum Choo ◽  
Daniel Autrey ◽  
Mohamed Rishard ◽  
Stephen Drucker ◽  
...  

The S1(n,π*) ← S0 cavity ringdown spectrum of 2-cyclohexen-1-one vapor has been recorded in the vicinity of the 000 band, which is at 26 089.1 cm–1. Observation of hot bands in the spectrum has permitted the determination of several low-frequency fundamentals and overtones in the ground electronic state. The lowest two excited quantum states for the inversion vibration (v39) were found to be at 99.0 and 197.0 cm–1. Together with previously published far-IR spectra and vapor-phase Raman spectra, the fundamental frequencies for v39, v38, and v37 have been determined. From observed v39 levels, the barrier to inversion has been determined experimentally to be 1900 ± 300 cm–1, which is very different from values of 935 and 3379 cm–1 previously reported from Raman and far-IR data, respectively. Density functional calculations carried out in this paper give a barrier value of 2090 cm-1 when the B3LYP/6-311+G(d,p) basis set is used.Key words: cavity ringdown spectra, 2-cyclohexen-1-one, Raman spectra, potential energy function, inversion barrier.


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