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High-frequency, limiting-phonon

In the time-domain detection of the vibrational coherence, the high-wavenumber limit of the spectral range is determined by the time width of the pump and probe pulses. Actually, the highest-wavenumber band identified in the time-domain fourth-order coherent Raman spectrum is the phonon band of Ti02 at 826 cm. Direct observation of a frequency-domain spectrum is free from the high-wavenum-ber limit. On the other hand, the narrow-bandwidth, picosecond light pulse will be less intense than the femtosecond pulse that is used in the time-domain method and may cause a problem in detecting weak fourth-order responses. [Pg.112]

The similarity between the A C o spectra doped with different alkali metals again indicates that the observed modes are due only to the Cfio molecule, and that there are no observable A-Cfto modes above 100 cm The mode at 270 cm has a resolution-limited FWHM for CSftCfio, is broadened in nd is a doublet in K C q. The high-frequency mode of the doublet may result from a two-phonon process involving a low cnergy-A-Cfrequency modes (1383 cm and 1478 cm ). If this is the case, it is not clear that these modes should be broadened in the same way as the... [Pg.168]

The phonon frequencies Vpho on in proteins have the following characteristic values at acoustic modes they lie between 10" and 10" s" ( 0.0004-0.004 eV) in a polypeptide chain the acoustic modes are generated by vibrations, which cause changes in the relative distances and orientations of the side chains. The upper limit is given by the high-frequency intramolecular vibrational modes of hydrogen atoms with a frequency of 10 s" ( 0.4 eV). At body temperatures (k T ks 310 K 0.03 eV), the acoustic modes will be most active in the scattering of electrons. Therefore for the subsequent considerations Vphonon = 10 s has been taken as the characteristic value. [Pg.352]


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Frequency limits

High frequencies

High limitations

High limiters

High-3-limit

High-frequency limit

Phonon frequency

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