The A Matrix in Molecular Vibration–Rotation Theory

Crawford's A matrix in the theory of molecular vibrations is, in a sense, the inverse of Wilson's B matrix, but is not unique because B is rectangular. We consider the general form of A and then use the Eckart conditions to obtain the solution A = M−1BTG−1, which has been widely used. Alth...

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Published in:Journal of molecular spectroscopy Vol. 205; no. 2; pp. 227 - 231
Main Authors: Winnewisser, Brenda P., Watson, James K.G.
Format: Journal Article
Language:English
Published: United States Elsevier Inc 01-02-2001
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Summary:Crawford's A matrix in the theory of molecular vibrations is, in a sense, the inverse of Wilson's B matrix, but is not unique because B is rectangular. We consider the general form of A and then use the Eckart conditions to obtain the solution A = M−1BTG−1, which has been widely used. Although the internal-coordinate harmonic force constants f = ATFXA, where FX are the Cartesian force constants, are superficially isotope-dependent, we show that this dependence vanishes. More generally, solutions of the form A = WBT(BWBT)−1, where W is an arbitrary nonsingular square matrix, are shown to give an f matrix that is independent of W.
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ISSN:0022-2852
1096-083X
DOI:10.1006/jmsp.2000.8268