2008
DOI: 10.1134/s1063776108010032
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Intramolecular vibrational dynamics of propyne and its derivatives: The role of vibrational-rotational mixing

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Cited by 13 publications
(16 citation statements)
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“…The knowledge of this quantity makes it possible to estimate the density of states of the molecule that are efficient with respect to the IVR process. In ref (see also refs and ), a universal function has been calculated, which describes the dependence of σ on the product x = ℏ W ρ, where W is the initial rate of decay from the initial state to the ensemble of states with the density ρ that obey the statistics of the Gaussian orthogonal ensemble (GOE), which is typical for the dynamic chaos range. , From the viewpoint of the model that was considered in the preceding subsection, it is interesting to consider the question about the density ρ A of states bold-scriptA , which are efficient with respect to the first, fast, stage of the IVR process. In terms of eq , the dilution factor that characterizes this stage is estimated as σ normalΓ normalA normalI normalΓ normalI normalA + normalΓ normalA normalI = 1 normalΓ normalI normalB ( τ 1 + τ 2 Γ I B τ 1 τ 2 ) where expression is used.…”
Section: Discussionmentioning
confidence: 99%
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“…The knowledge of this quantity makes it possible to estimate the density of states of the molecule that are efficient with respect to the IVR process. In ref (see also refs and ), a universal function has been calculated, which describes the dependence of σ on the product x = ℏ W ρ, where W is the initial rate of decay from the initial state to the ensemble of states with the density ρ that obey the statistics of the Gaussian orthogonal ensemble (GOE), which is typical for the dynamic chaos range. , From the viewpoint of the model that was considered in the preceding subsection, it is interesting to consider the question about the density ρ A of states bold-scriptA , which are efficient with respect to the first, fast, stage of the IVR process. In terms of eq , the dilution factor that characterizes this stage is estimated as σ normalΓ normalA normalI normalΓ normalI normalA + normalΓ normalA normalI = 1 normalΓ normalI normalB ( τ 1 + τ 2 Γ I B τ 1 τ 2 ) where expression is used.…”
Section: Discussionmentioning
confidence: 99%
“…A simple phenomenological model that is based on kinetic equations for the populations N I and N A is considered in the Appendix. (The usage of the rate equations is justified with a good accuracy because in our experimental conditions we deal with very large ensembles of initial vibrational–rotational states (see, e.g., results of model calculations based on the Schrödinger equation and presented in refs and ).) In accordance with the notation of Figure , unknown rates of the forward and backward processes bold-scriptI bold-scriptA are introduced: Γ I→A and Γ A→I .…”
Section: Discussionmentioning
confidence: 99%
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“…The relation between W, σ, and ρ eff will be clarified in section 2. As a useful example, this relation made it possible to establish that, for some molecules, the IVR spreads on not only all accessible vibrational states (with the possible exclusion of the torsion modes [10]), but, what matters much more for the value of ρ eff , the IVR occurs without conservation of the rotational quantum number K in cases of symmetric-top molecules, or K a in cases of asymmetric tops (see [11][12][13][14][15][16][17] for details).…”
Section: Photon Echoes For Studying Intramolecular Vibrational Redist...mentioning
confidence: 99%
“…Due to the high pressure and the slow relaxation process collisional effects could not be excluded in these earlier experiments 57 (see also ref. [60][61][62].…”
Section: Introductionmentioning
confidence: 99%