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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Abstract 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.
AbstractList 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(-1)B(T)G(-1), which has been widely used. Although the internal-coordinate harmonic force constants f = A(T)F(X)A, where F(X) are the Cartesian force constants, are superficially isotope-dependent, we show that this dependence vanishes. More generally, solutions of the form A = WB(T)(BWB(T))(-1), where W is an arbitrary nonsingular square matrix, are shown to give an f matrix that is independent of W. Copyright 2001 Academic Press.
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.
Author Winnewisser, Brenda P.
Watson, James K.G.
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  givenname: James K.G.
  surname: Watson
  fullname: Watson, James K.G.
  organization: Steacie Institute for Molecular Sciences, National Research Council of Canada, Ottawa, Ontario, Canada, K1A 0R6
BackLink https://www.ncbi.nlm.nih.gov/pubmed/11162208$$D View this record in MEDLINE/PubMed
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Cites_doi 10.1063/1.1740158
10.1063/1.1750829
10.1021/jp993430o
10.1016/0022-2852(87)90053-1
10.1063/1.1700660
10.1063/1.1742730
10.1016/0022-2860(93)08009-S
10.1103/PhysRev.47.552
10.1016/0022-2852(75)90294-5
10.1063/1.1747981
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Keywords A matrix
internal coordinates
force constants
ab initio force fields
Cartesian coordinates
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Fogarasi (10.1006/jmsp.2000.8268_RF8) 1985
Wilson (10.1006/jmsp.2000.8268_RF2) 1980
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Snippet 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...
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SubjectTerms A matrix
ab initio force fields
Cartesian coordinates
force constants
internal coordinates
Title The A Matrix in Molecular Vibration–Rotation Theory
URI https://dx.doi.org/10.1006/jmsp.2000.8268
https://www.ncbi.nlm.nih.gov/pubmed/11162208
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Volume 205
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