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Coupling, vibrational

Pekeris C L 1934 The rotation-vibration coupling in diatomic molecules Phys. Rev. 45 98 Slater J C and Kirkwood J G 1931 The van der Waals forces in gases Phys. Rev. 37 682... [Pg.216]

The fonn of the classical (equation C3.2.11) or semiclassical (equation C3.2.11) rate equations are energy gap laws . That is, the equations reflect a free energy dependent rate. In contrast with many physical organic reactivity indices, these rates are predicted to increase as -AG grows, and then to drop when -AG exceeds a critical value. In the classical limit, log(/cg.j.) has a parabolic dependence on -AG. Wlren high-frequency chemical bond vibrations couple to the ET process, the dependence on -AG becomes asymmetrical, as mentioned above. [Pg.2982]

Band 8, 7-lOy. (1408 cm. ). This is a characteristic carboxybc acid absorption band and it arises from a C—0 vibration coupled with an... [Pg.1140]

Treating the full internal nuclear-motion dynamics of a polyatomic molecule is complicated. It is conventional to examine the rotational movement of a hypothetical "rigid" molecule as well as the vibrational motion of a non-rotating molecule, and to then treat the rotation-vibration couplings using perturbation theory. [Pg.342]

C—F 1400-870 Correlations of limited applicability because of vibrational coupling with stretching... [Pg.775]

Fig. 17. Contour plots for a Fig. 17. Contour plots for a <j vibration coupled symmetrically (left) and antisymmetrically (right) to the reaction coordinate Q. The cross indicates the saddle point. Lines 1, 2 and 3 correspond to MEP, sudden trajectory, and to the path in the static barrier. Below a sketch of the potential along the tunneling coordinate Q is represented at different < .
Fig. 31. Two-dimensional periodic orbits for vibration coupled antisymmetrically to the reaction coordinate. Caustics (C) and take-off points (T) are indicated. Fig. 31. Two-dimensional periodic orbits for vibration coupled antisymmetrically to the reaction coordinate. Caustics (C) and take-off points (T) are indicated.
As argued in section 2.3, when the asymmetry e far exceeds A, phonons should easily destroy coherence, and relaxation should persist even in the tunneling regime. Such an incoherent tunneling, characterized by a rate constant, requires a change in the quantum numbers of the vibrations coupled to the reaction coordinate. In section 2.3 we derived the expression for the intradoublet relaxation rate with the assumption that only the one-phonon processes are relevant. [Pg.102]

Fig. 56. Contour plots of (a) shaking and (b) breathing vibrations coupled to hindered rotation around the three-fold axis. The MEP is shown. Fig. 56. Contour plots of (a) shaking and (b) breathing vibrations coupled to hindered rotation around the three-fold axis. The MEP is shown.
Increasing vibration with speed. Vibration Coupling damage Pitting of coupling teeth... [Pg.426]

RAIRS spectra contain absorption band structures related to electronic transitions and vibrations of the bulk, the surface, or adsorbed molecules. In reflectance spectroscopy the ahsorhance is usually determined hy calculating -log(Rs/Ro), where Rs represents the reflectance from the adsorhate-covered substrate and Rq is the reflectance from the bare substrate. For thin films with strong dipole oscillators, the Berre-man effect, which can lead to an additional feature in the reflectance spectrum, must also be considered (Sect. 4.9 Ellipsometry). The frequencies, intensities, full widths at half maximum, and band line-shapes in the absorption spectrum yield information about adsorption states, chemical environment, ordering effects, and vibrational coupling. [Pg.251]

Bratos S., Chestier J. P. Infrared and Raman study of liquids. III. Theory of rotation-vibration coupling effects. Diatomic molecules in inert solutions, Phys. Rev. A9, 2136-50 (1974). [Pg.285]

From an energetic point of view, the bands at higher wavenumbers can be assigned to the Ss rings. However, the intensities were found as ca. 0.65 1 (pure infected) instead of 2.8 1 which would be expected from the natural abundance of the isotopomers. These discrepancies were solved by applying the mathematical formalism utilized in the treatment of intramolecular Fermi resonance (see, e.g., [132]). Accordingly, in the natural crystal we have to deal with vibrational coupling between isotopomers in the primitive cell of the crystal [109]. [Pg.61]

In EMIRS and SNIFTIRS measurements the "inactive" s-polarlsed radiation is prevented from reaching the detector and the relative intensities of the vibrational bands observed in the spectra from the remaining p-polarised radiation are used to deduce the orientation of adsorbed molecules. It should be pointed out, however, that vibrational coupling to adsorbate/adsorbent charge transfer (11) and also w electrochemically activated Stark effect (7,12,13) can lead to apparent violations of the surface selection rule which can invalidate simple deductions of orientation. [Pg.552]

Equation 1 describes the radiationless decay rate for a single-frequency model with weak electron-vibration coupling in the low temperature limit as derived by Englman and Jortner. [Pg.498]

It was noted early by Reed and others that the IETS spectrum could exhibit both absorption and emission peaks - that is, the plots of Fig. 9 could have positive excursions and negative excursions called peaks and dips. The simple analysis suggested in Fig. 9 implies that it should always be absorptive behavior, and therefore that there should always be a peak (a maximum, an enhancement) in the IETS spectrum at the vibrational resonances. It has been observed, however, that dips sometimes occur in these spectra. These have been particularly visible in small molecules in junctions, such as in the work of van Ruitenbeek [92, 109] (Fig. 12). Here, formal analysis indicates that, as the injection gap gets smaller, the existence of an inelastic vibrational channel does not contribute a second independent channel to the transport, but rather opens up an interference [100]. This interference can actually impede transport, resulting in a dip in the spectrum. Qualitatively, this occurs because the system is close to an electronic resonance without the vibrational coupling the conductance is close to g0, and the interference subtracts from the current. [Pg.21]

The reorganization free energy /.R represents the electronic-vibrational coupling, ( and y are fractions of the overpotential r] and of the bias voltage bias at the site of the redox center, e is the elementary charge, kB the Boltzmann constant, and coeff a characteristic nuclear vibration frequency, k and p represent, respectively, the microscopic transmission coefficient and the density of electronic levels in the metal leads, which are assumed to be identical for both the reduction and the oxidation of the intermediate redox group. Tmax and r max are the current and the overvoltage at the maximum. [Pg.173]

Torsional flexing and related torsion-vibration-coupling effects... [Pg.243]

HB-3) pronounced three-center character, with distinctive 2 Jab geminal spin couplings, IR vibrational couplings, and other spectroscopic signatures ... [Pg.282]


See other pages where Coupling, vibrational is mentioned: [Pg.3012]    [Pg.347]    [Pg.16]    [Pg.26]    [Pg.259]    [Pg.293]    [Pg.299]    [Pg.168]    [Pg.560]    [Pg.560]    [Pg.383]    [Pg.387]    [Pg.119]    [Pg.152]    [Pg.153]    [Pg.89]    [Pg.35]    [Pg.48]    [Pg.83]    [Pg.497]    [Pg.95]    [Pg.226]    [Pg.244]    [Pg.301]   
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Vibration coupled

Vibrations, coupling

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