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Medium-frequency vibrational mode

Figure 2 Emission spectrum fit with Equation (1). The value of E, the average of medium frequency vibrational modes contributing to nonradiative relaxation, ht/, the degree of excited state distortion, proportional to the Huang Rhys factor S, and the degree of inhomogeneous broadening of vibronic... Figure 2 Emission spectrum fit with Equation (1). The value of E, the average of medium frequency vibrational modes contributing to nonradiative relaxation, ht/, the degree of excited state distortion, proportional to the Huang Rhys factor S, and the degree of inhomogeneous broadening of vibronic...
Recently Tanimura and Mukamel have proposed a fifth order nonlinear spectroscopy that is capable of distinguishing homogeneous and inhomogeneous contributions to low frequency vibrational modes. 1 As shown in Fig. 1, a medium interacts with two pairs of short pulses with the same wavelength at... [Pg.390]

For these multi-mode processes it is still possible to employ the average-mode approximation [27,30], and take S as the sum of the Sj values for the coupled high- and medium-frequency vibrations... [Pg.418]

The rates were calculated according to TM-1 assuming the following approximations (i) near adiabaticity (Kj,j 1) (ii) dielectric continuum model for the solvent (iii) intermediate distortions between oxidised and reduced species for the internal modes and (iv) separation between internal modes and medium modes (either high-frequency vibrational modes or low frequency). This last approximation is implicit in eqs. (16.12)-(16.15). The separation between the inner-sphere, AG/, and the outer-sphere, AGf, reorganisation... [Pg.441]

From that value a force constant of k = 5.6 mdynA 1 for the Si=C double bond is deduced255. This frequency is clearly higher than the usual range for Si—C stretch vibrations but substantially less than for C=C stretches, both because Si is heavier than C and because the Si=C bond is weaker than the C=C bond. More suitable for the experimental characterization is the vinylic Si—H stretch vibration which gives rise to a medium band at 2239 cm-1 (25) or 2187 cm-1 (2)29, hypsochromically shifted by around 100 cm-1 relative to the Si—H stretch in simple silanes. A detailed analysis of the vibrational spectra of matrix-isolated MeHSi=CH2 26 using polarized IR spectroscopy established IR transition moment directions relative to the tot -transition moment (Si-C axis) in 26156. These data provide detailed information about the vibrational modes and about the structure of 26156. The bathochromic shift of the Si=C stretch in the isomeric 1,3-silabuta-l,3-dienes 289 and 290 by around 70 cm 1 compared with the Si=C stretch in simple silenes (Table 15), was interpreted as an indication of Si=C—C=C and C=Si—C=C 7r-conjugation159. [Pg.995]

As already discussed in Section 13.1, the multiphonon pathway for vibrational relaxation is a relatively slow relaxation process, and, particularly at low temperatures the system will use other relaxation routes where accessible. Polyatomic molecules take advantage of the existence of relatively small frequency differences, and relax by subsequent medium assisted vibrational energy transfer between molecular modes. Small molecules often find other pathways as demonstrated in Section 13.1 for the relaxation ofthe CN radical. When the concentration of impurity molecules is not too low, intermolecular energy transfer often competes successfully with local multiphonon relaxation. For example, when a population of CO molecules in low temperature rare gas matrices is excited to the v = 1 level, the system takes advantage ofthe molecular anhannomcity by undergoing an intermediate relaxation of the type... [Pg.476]

A relatively new method for studying chemisorbed species is sum-frequency generation (SFG) (see Table 4.1 for references). This is a second-order non-linear process, requiring both a fixed visible and a tuneable laser the selection rules determine that a vibrational mode must result in changes both to dipole moment and to polarisability for the effect to occur, and this limits it to a medium which lacks inversion symmetry, i.e. to the surface and not the gas phase. This, coupled with the fact that excitation is by photons, not electrons, leads to the inestimable benefit of being usable in the presence of a high gas pressure, and therefore enables in situ examination of the surface under reaction conditions. [Pg.160]


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Medium frequency

Vibration frequency

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