Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Intramolecular vibrational energy time dependent

The second part of the chapter (Section III) deals with the time-dependent self-consistent-field (TDSCF) method for studying intramolecular vibrational energy transfer in time. The focus is both on methodological aspects and on the application to models of van der Waals cluster systems, which exhibit non-RRKM type of behavior. Both Sections II and III review recent results. However, some of the examples and the theoretical aspects are presented here for the first time. [Pg.99]

The first step in a unimolecular reaction involves energizing the reactant molecule above its decomposition threshold. An accurate description of the ensuing unimolecular reaction requires an understanding of the state prepared by this energization process. In the first part of this chapter experimental procedures for energizing a reactant molecule are reviewed. This is followed by a description of the vibrational/rotational states prepared for both small and large molecules. For many experimental situations a superposition state is prepared, so that intramolecular vibrational energy redistribution (IVR) may occur (Parmenter, 1982). IVR is first discussed quantum mechanically from both time-dependent and time-independent perspectives. The chapter ends with a discussion of classical trajectory studies of IVR. [Pg.67]

The concept of intramolecular vibrational energy redistribution (IVR) can be formulated from both time-dependent and time-independent viewpoints (Li et al., 1992 Sibert et al., 1984a). IVR is often viewed as an explicitly time-dependent phenomenon, in which a nonstationary superposition state, as described above, is initially prepared and evolves in time. Energy flows out of the initially excited zero-order mode, which may be localized in one part of the molecule, to other zero-order modes and, consequently, other parts of the molecule. However, delocalized zero-order modes are also possible. The nonstationary state initially prepared is often referred to as the bright state, as it carries oscillator strength for the spectroscopic transition of interest, and IVR results in the flow of amplitude into the manifold of so-called dark states that are not excited directly. It is of interest to understand what physical interactions couple different zero-order modes, allowing energy to flow between them. A particular type of superposition state that has received considerable study are A/-H local modes (overtones), where M is a heavy atom (Child and Halonen, 1984 Hayward and Henry, 1975 Watson et al., 1981). [Pg.81]

We demonstrated that the field-induced large amplitude vibration of the hg(l) mode persists for a rather long period (a few to several picoseconds), owing to slow intramolecular vibrational energy redistribution (IVR) [28]. Mode selective excitation can therefore be achieved by adjusting the pulse intervals in a pulse train [24], as in the experiment reported by Laarmann et al. [9]. In this chapter, by using the time-dependent adiabatic state approach, we first demonstrate that... [Pg.152]

If the time interval between the formation of the activated intermediate complex and the collision for stabilization is long compared to the lifetime (r, Hk of the intermediate product, (A+M)+, the activated complex will decompose back to the initial reactants. Since the formation of the association products depends on the collision with the third-body gas molecules (N), the entire process is a competition between intermolecular collisional energy transfer and intramolecular vibrational energy redistribution of the excess energy of the activated intermediate complex among its degrees of freedom. [Pg.22]

For the case of intramolecular energy transfer from excited vibrational states, a mixed quantum-classical treatment was given by Gerber et al. already in 1982 [101]. These authors used a time-dependent self-consistent field (TDSCF) approximation. In the classical limit of TDSCF averages over wave functions are replaced by averages over bundles of trajectories, each obtained by SCF methods. [Pg.16]

R.B. Gerber, V. Buch and M.A. Ratner, Time-dependent self-consistent field approximation for intramolecular energy transfer. I. Formulation and application to dissociation of van der Waals molecules, J. Chem. Phys., 77 (1982), 3022 M.A. Ratner and R.B. Gerber, Excited vibrational states of polyatomic molcecules the semiclassical self-consistent field approach, J. Phys. Chem., 90 (1986) 20 R.B. Gerber and M.A. Ratner, Mean-field models for molecular states and dynamics new developments, J. Phys. Chem., 92 (1988) 3252 ... [Pg.155]


See other pages where Intramolecular vibrational energy time dependent is mentioned: [Pg.820]    [Pg.854]    [Pg.181]    [Pg.352]    [Pg.526]    [Pg.113]    [Pg.122]    [Pg.453]    [Pg.820]    [Pg.854]    [Pg.181]    [Pg.307]    [Pg.457]    [Pg.567]    [Pg.194]    [Pg.212]    [Pg.64]    [Pg.144]    [Pg.879]    [Pg.181]    [Pg.443]    [Pg.267]    [Pg.299]    [Pg.54]    [Pg.140]    [Pg.34]    [Pg.18]    [Pg.126]    [Pg.349]    [Pg.325]    [Pg.145]    [Pg.563]    [Pg.181]    [Pg.331]    [Pg.24]    [Pg.39]    [Pg.119]    [Pg.121]    [Pg.193]    [Pg.318]    [Pg.38]    [Pg.194]   
See also in sourсe #XX -- [ Pg.81 ]




SEARCH



Energy vibrational

Energy-dependent

Intramolecular vibrational

Intramolecular vibrational energy

Intramolecular vibrations

Intramolecular vibrations, energy

Vibration energy

Vibration time

© 2024 chempedia.info