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 |
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Main Authors: | , |
Format: | Journal Article |
Language: | English |
Published: |
United States
Elsevier Inc
01-02-2001
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Subjects: | |
Online Access: | Get full text |
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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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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0022-2852 1096-083X |
DOI: | 10.1006/jmsp.2000.8268 |