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Intramolecular vibrational-rotational energy transfer

Collision-induced intramolecular vibration-to-rotation energy transfer appears to be inefficient. The evidence for this inference comes from the study of rotational contours in the one collision-induced transition 7 0° in glyoxal. It is found that the emission from 0° has a distribution over rotational transitions that is close to the thermal distribution. But the vibration v-j in glyoxal is a torsional motion, and the axis of torsion very nearly coincides with the smallest axis of inertia of the molecule, so if collision-induced intramolecular vibra-tion-to-rotation transfer were efficient the emission from 0 should have a nonthermal distribution in the quantum number K (which describes quantization of the motion about the smallest axis of inertia). Note, however, that the collision partner used in this experiment was... [Pg.259]

This is no longer the case when (iii) motion along the reaction patir occurs on a time scale comparable to other relaxation times of the solute or the solvent, i.e. the system is partially non-relaxed. In this situation dynamic effects have to be taken into account explicitly, such as solvent-assisted intramolecular vibrational energy redistribution (IVR) in the solute, solvent-induced electronic surface hopping, dephasing, solute-solvent energy transfer, dynamic caging, rotational relaxation, or solvent dielectric and momentum relaxation. [Pg.831]

Figure 3.10 Vibrational deexcitation of a classical Morse oscillator as a function of the orientation angle fl0 (see text), according to Kelley [98], for the case mA + mB mc = 2 + 1 - 1. Rotational energy is acquired via intramolecular V—R transfer. AirT0T is the net internal energy lost by the molecule BC. Figure 3.10 Vibrational deexcitation of a classical Morse oscillator as a function of the orientation angle fl0 (see text), according to Kelley [98], for the case mA + mB mc = 2 + 1 - 1. Rotational energy is acquired via intramolecular V—R transfer. AirT0T is the net internal energy lost by the molecule BC.
It is instructive to examine a zeroth-order calculation of intramolecular energy transfer in a model molecule in which the energies of the vibrational and rotational modes are conserved separately, in which the initial excitation of the van der Waals stretching mode is zero (n = 0), and in which the initial values of... [Pg.48]

INTRAMOLECULAR dynamics is the time evolution of rotational, vibrational, and electronic degrees of freedom of isolated individual molecules, that is, molecules in a collision-free environment. As in any mechanical system, one can consider the time evolution of any of a variety of system properties. Intramolecular energy transfer focuses... [Pg.118]


See other pages where Intramolecular vibrational-rotational energy transfer is mentioned: [Pg.349]    [Pg.349]    [Pg.1049]    [Pg.1049]    [Pg.53]    [Pg.219]    [Pg.1025]    [Pg.1047]    [Pg.158]    [Pg.192]    [Pg.190]    [Pg.130]    [Pg.696]    [Pg.12]    [Pg.205]    [Pg.312]    [Pg.35]    [Pg.41]    [Pg.72]    [Pg.18]    [Pg.36]    [Pg.442]    [Pg.30]    [Pg.1]    [Pg.12]    [Pg.105]    [Pg.442]    [Pg.1025]    [Pg.1047]    [Pg.244]    [Pg.259]    [Pg.190]    [Pg.37]    [Pg.155]    [Pg.175]    [Pg.102]    [Pg.162]    [Pg.176]    [Pg.85]    [Pg.217]    [Pg.358]    [Pg.84]    [Pg.341]   
See also in sourсe #XX -- [ Pg.349 ]




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Energy rotational

Energy transfer vibration-rotation

Energy vibrational

Intramolecular vibrational

Intramolecular vibrational energy

Intramolecular vibrational energy transfer

Intramolecular vibrational-rotational energy

Intramolecular vibrations

Intramolecular vibrations, energy

Rotating energy

Rotation energy

Rotation energy transfer

Rotation-vibration

Rotational transfer

Rotational vibrations

Rotational-vibrational

Rotational-vibrational energy transfer

Vibrating rotator

Vibration Transfer

Vibration energy

Vibrational energy transfer

Vibrational transfer

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