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Vibrational level coupling

The observation of novel quantum beats in the spectrally resolved fluorescence of anthracene21 forced one to consider, within the context of radiationless transition theory, the details of how IVR might be manifested in beat-modulated fluorescence decays. This work led to the concepts of phase-shifted quantum beats and restricted IVR,30a,4° and to a general set of results306 pertaining to the decays of spectrally resolved fluorescence in situations where an arbitrary number of vibrational levels, coupled by anharmonic coupling, participate in IVR. Moreover, three regimes of IVR have been identified no IVR, restricted (or coherent) IVR, and dissipative IVR.42... [Pg.277]

The only tenn in this expression that we have not already seen is a, the vibration-rotation coupling constant. It accounts for the fact that as the molecule vibrates, its bond length changes which in turn changes the moment of inertia. Equation B1.2.2 can be simplified by combming the vibration-rotation constant with the rotational constant, yielding a vibrational-level-dependent rotational constant. [Pg.1153]

For quantitative work, it is necessary to include anhaniionic corrections and coupling between tlie nonnal modes, but tlie general picture suffices to handle tlie lower vibrational levels of most near-rigid molecules. [Pg.2444]

It is possible that the driven equipment to which the motor is coupled has a higher vibration level than the motor, resulting in quantum imbalance and more vibrations than when the motor was tested. All attempts must be made, to bring the vibration level of the drive and the driven system within the limits as prescribed in Table 11.3. [Pg.240]

The situation is more subtle for the antisymmetrically coupled mode. As shown in fig. 17, this vibration, in contrast to the symmetric mode, asymmetrizes the potential and violates the resonance. This should lead to a decrease in the splitting. Consider this problem perturbatively. If the vibration and the potential V Q) were uncoupled, each tunneling doublet Eq, Ei (we consider only the lowest one) of the uncoupled potential V Q) would give rise to a progression of vibrational levels with energies... [Pg.37]

Fig. 8. Scattering the transition state from the surface. Measured vibrational distribution of NO resulting from scattering of laser-prepared NO(v = 15) from Au (111) at incidence = 5 kJ mol-1. Only a small fraction of the laser-prepared population of v = 15 remains in the initial vibrational state. The most probable scattered vibrational level is more than 150 kJ mol-1 lower in energy than the initial state. Vibrational states below v = 5 could not be detected due to background problems. These experiments provide direct evidence that the remarkable coupling of vibrational motion to metallic electrons postulated by Luntz et al. can in fact occur. (See Refs. 44 and 59.)... Fig. 8. Scattering the transition state from the surface. Measured vibrational distribution of NO resulting from scattering of laser-prepared NO(v = 15) from Au (111) at incidence = 5 kJ mol-1. Only a small fraction of the laser-prepared population of v = 15 remains in the initial vibrational state. The most probable scattered vibrational level is more than 150 kJ mol-1 lower in energy than the initial state. Vibrational states below v = 5 could not be detected due to background problems. These experiments provide direct evidence that the remarkable coupling of vibrational motion to metallic electrons postulated by Luntz et al. can in fact occur. (See Refs. 44 and 59.)...
It is useful to view optical absorption and emission processes in such a system in terms of transitions between distinct vibrational levels of the ground and excited electronic states of a metal atom-rare gas complex or quasi-molecule. Since the vibrational motions of the complex are coupled with the bulk lattice vibrations, a complicated pattern of closely spaced vibrational levels is involved and this results in the appearance of a smooth, structureless absorption profile (25). Thus the homogeneous width of the absorption band arises from a coupling between the electronic states of the metal atom and the host lattice vibrations, which is induced by the differences between the guest-host... [Pg.299]

Description Coupled to a Block-Davidson Algorithm An Efficient Scheme to Calculate Highly Excited Vibrational Levels. [Pg.344]

The energy Ea is a quantum term associated with the proton reaction coordinate coupling to the Q vibration, Ea = h1 /2m. and Co is the tunneling matrix element for the transfer from the 0th vibrational level in the reactant state to the 0th vibrational level in the product state. The term AQe is the shift in the oscillator equilibrium position and F L(Eq, Ea, Laguerre polynomial. For a thorough discussion of Eq. (8), see [13],... [Pg.77]

Adapted from Shao, Walet and Amado, 1992. For CO2, Fermi couplings have been included. The quantum numbers for each vibrational level are in their usual order, v, vj,. ... [Pg.185]


See other pages where Vibrational level coupling is mentioned: [Pg.1143]    [Pg.129]    [Pg.476]    [Pg.492]    [Pg.492]    [Pg.492]    [Pg.501]    [Pg.552]    [Pg.603]    [Pg.112]    [Pg.36]    [Pg.128]    [Pg.473]    [Pg.300]    [Pg.997]    [Pg.293]    [Pg.88]    [Pg.350]    [Pg.403]    [Pg.410]    [Pg.410]    [Pg.411]    [Pg.145]    [Pg.494]    [Pg.140]    [Pg.710]    [Pg.914]    [Pg.80]    [Pg.233]    [Pg.584]    [Pg.600]    [Pg.600]    [Pg.600]    [Pg.609]    [Pg.660]    [Pg.711]    [Pg.10]    [Pg.355]    [Pg.292]    [Pg.137]   
See also in sourсe #XX -- [ Pg.334 ]




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