1996
DOI: 10.1006/aphy.1996.0129
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A General Algebraic Model for Molecular Vibrational Spectroscopy

Abstract: We introduce the Anharmonic Oscillator Symmetry Model to describe vibrational excitations in molecular systems exhibiting high degree of symmetry. A systematic procedure is proposed to establish the relation between the algebraic and configuration space formulations, leading to new interactions in the algebraic model. This approach incorporates the full power of group theoretical techniques and provides reliable spectroscopic predictions.We illustrate the method for the case of D 3h -triatomic molecules.1

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Cited by 80 publications
(72 citation statements)
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“…Physically, these contributions arise from the anharmonic character of the interatomic interactions, and seem to play an important role when dealing with molecular anharmonicities, especially at higher number of quanta. This conclusion is supported by our other applications of the symmetry-adapted model to the Be 4 cluster [16] and the H + 3 , Be 3 and Na + 3 molecules [19], as well as our study of two isotopes of the ozone molecule [20].…”
Section: Discussionsupporting
confidence: 74%
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“…Physically, these contributions arise from the anharmonic character of the interatomic interactions, and seem to play an important role when dealing with molecular anharmonicities, especially at higher number of quanta. This conclusion is supported by our other applications of the symmetry-adapted model to the Be 4 cluster [16] and the H + 3 , Be 3 and Na + 3 molecules [19], as well as our study of two isotopes of the ozone molecule [20].…”
Section: Discussionsupporting
confidence: 74%
“…(13,15) and carry out the building up procedure to construct the Hamiltonian and states with a higher number of quanta with the appropriate projection operators and Clebsch-Gordan coefficients [19].…”
Section: H Triatomic Moleculesmentioning
confidence: 99%
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“…In particular, a one-to-one correspondence can be established between eigenstates of the Morse-Schrödinger equation, h͉͘ϭ͉͘ with hϭ p 2 /2m ϩV(x), and the representations of U(2), ͉N,͘, the latter being characterized by two quantum numbers which specify the total number of bound levels, 1ϩN/2 or 1ϩ(NϪ1)/2 ͑N even or N odd͒, and the vibrational index, , such that ϭ0,1...N/2 or (NϪ1)/2. When recast in the U(2) basis, the Morse Hamiltonian assumes the simple form hϭ 0 ϩAC where 0 and A signify constant modeling parameters while C is related to the invariant quadratic Casimir operator C of the subalgebra O(2) ͓with eigenvalues m 2 ϭ(NϪ2) 2 ͔ by means of: 65,66 Cϭ…”
Section: Lie Algebraic Analyses a Lie Algebraic Realization Of Tmentioning
confidence: 99%
“…However, in molecular systems, if the Hamiltonian goes beyond one and two-body operators, the number of interactions is greater than the number of invariant operators [59]. Consequently another prescription should be used to construct the Hamiltonian.…”
Section: Algebraic Approach To Triatomic Moleculesmentioning
confidence: 99%