1986
DOI: 10.1063/1.451574
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Vibrational energy transfer and migration processes in matrix isolated CH3F

Abstract: Following excitation ofthe V3 mode in matrix isolated CH 3 F, population of 2V3 is observed. Population of2v3 occurs via intermolecular vibration-vibration (V-V) energy transfer driven by the exothermicity of the anharmonic V -V step equilibrating these states. In the equilibration process, both resonant and nonresonant intermolecular energy transfer processes have been identified. The probabilities of each of these processes have been determined. The phonon assisted nonresonant V-V process has a probability o… Show more

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Cited by 13 publications
(4 citation statements)
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“…We label these {q i } i)1 6 in the following sequence: symmetric stretch (water one), asymmetric stretch (water one), bending (water one), and then the three NMs for water number two in a similar sequence. The remaining coordinates, {q i } i) 7 18 , are the standard center of mass coordinates and Euler angles for each molecule. The values of all 18 coordinates are chosen so as to reproduce the dimer equilibrium geometry.…”
Section: Why a Harmonic Model Should Workmentioning
confidence: 99%
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“…We label these {q i } i)1 6 in the following sequence: symmetric stretch (water one), asymmetric stretch (water one), bending (water one), and then the three NMs for water number two in a similar sequence. The remaining coordinates, {q i } i) 7 18 , are the standard center of mass coordinates and Euler angles for each molecule. The values of all 18 coordinates are chosen so as to reproduce the dimer equilibrium geometry.…”
Section: Why a Harmonic Model Should Workmentioning
confidence: 99%
“…This fully determines their value, up to an irrelevant value of the whole dimer center of mass coordinates and Euler angles. Afterward, the coordinates {q i } i) 7 18 are frozen at their specific values, to make things simple, not because it is essential for the argument. The dimer intermolecular potential energy can now be Taylor-expanded in the six vibrational NMs around the minimum geometry of the dimer The lowest order term in this expansion, which induces an annihilation of one quantum of, say, symmetric stretch in water one (deactivating state |1〉 ≡ |100000〉) and creates a corresponding quantum in water two (activating state |2〉 ≡ |000100〉), is clearly the quadratic term V′ ≡ R 1,4 q 1 q 4 , since in terms of boson creation and annihilation operators this term equals (ref 30), where ω(sym) and m equal the monomer water symmetric stretch frequency and reduced mass, respectively.…”
Section: Why a Harmonic Model Should Workmentioning
confidence: 99%
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