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Symmetric stretching mode

We now compare the results calculated for the fundamental frequency of the symmetric stretching mode with the only available experimental datum [78] of 326 cm . The theoretical result is seen to exceed experiment by only 8.3%. It should be recalled that the Li3 and Li3 tiimers have for lowest J the values 0 and respectively. Thus, the istopic species Li3 cannot contribute to the nuclear spin weight in Eq. (64), since the calculations for half-integer J should employ different nuclear spin weights. Note that atomic masses have been used... [Pg.599]

Four IR absorption bands have been identified in the spectrum of the hydroxysulfonyl radical (HOSO 2) which has been obtained by the reaction of hydroxyl radicals with sulfur dioxide in argon matrix at 11 K16. The observed bands at 3539.9 and 759.5 cm 1 have been assigned to O—H and S—OH stretching modes while the bands at 1309.2 and 1097.3 cm-1 have been assigned to the asymmetric and symmetric stretching modes of the double bonded S02 moiety. These data are consistent with the theoretical prediction on the geometry of the hydroxysulfonyl radical12. [Pg.1094]

Without 2846-2850 CH2 symmetric stretching mode d crystalline PE with gauche-defect [131,133,146,147]... [Pg.142]

One major interest in vibrational surface spectroscopy is the ability to directly probe lipid layers. Similarly to the previous case, the structure of the alkyl chains of phospholipids is readily determined from the ratio of the magnitude of the CH2 and CH3 symmetrical stretching modes [136,137]. At the D2O-CCI4 interface, a layer of... [Pg.159]

To uniquely associate the unusual behavior of the collision observables with the existence of a reactive resonance, it is necessary to theoretically characterize the quantum state that gives rise to the Lorentzian profile in the partial cross-sections. Using the method of spectral quantization (SQ), it is possible to extract a Seigert state wavefunction from time-dependent quantum wavepackets using the Fourier relation Eq. (21). The state obtained in this way for J = 0 is shown in Fig. 7 this state is localized in the collinear F — H — D arrangement with 3-quanta of excitation in the asymmetric stretch mode, and 0-quanta of excitation in the bend and symmetric stretch modes. If the state pictured in Fig. 7 is used as an initial (prepared) state in a wavepacket calculation, one observes pure... [Pg.64]

Figure 9.22 Simple vibration modes for carbon dioxide, 0=C=0 (a) a symmetric stretching mode and (b) a scissor mode vibration... Figure 9.22 Simple vibration modes for carbon dioxide, 0=C=0 (a) a symmetric stretching mode and (b) a scissor mode vibration...
Fig. IS. Infrared absorption spectra of a full monolayer of H and D on W(IOO) at 100 K. The peak at 1070 (767)cm" is the symmetric stretch mode and the sharp peak at 1270 (915)cm is assigned to the second harmonic of the wag mode. The dotted line is calculated using the theory for an electron-hole pair damped mode by Langreth. Reproduced by permission from Chahat. )... Fig. IS. Infrared absorption spectra of a full monolayer of H and D on W(IOO) at 100 K. The peak at 1070 (767)cm" is the symmetric stretch mode and the sharp peak at 1270 (915)cm is assigned to the second harmonic of the wag mode. The dotted line is calculated using the theory for an electron-hole pair damped mode by Langreth. Reproduced by permission from Chahat. )...
The bridging position was further confirmed by the Li/ Li or C/ C isotopic shifts of the Li—C2H4 symmetrical stretching mode at 400 cm , which were too large and too small, respectively, for a simple C—Li oscillator. ... [Pg.239]

As was mentioned previously, the first absorption band (I) of 4a,4b-dihydrophen-anthrene is usually structureless and rather broad, having a half height width (AXiy2) of 4700 cm in 1. This band shows vibrational structure (developed to various extents) only in 12,13,15, 37, 38, 40, 43-46, and in 49—53 (see Table 13). The observed vibrational spacings, usually 1200—1400 cm correspond very probably to an excited state-totally symmetric stretching mode (i/j) of the C—C double bonds such as... [Pg.59]

FTIR has been mainly used to obtain structural details of films and to monitor intercalation of metal ions into the film structure and the subsequent reactions of the films with dihydrogen chalcogenides. Both transmission (FTIR-T) and reflection-absorbance (FTIR-RA) modes have been utilized. For the most part these studies have involved films of fatty acids with divalent metal ions. The key features of the FTIR spectra of these films include the asymmetric and symmetric stretching modes of the carboxylate group vs(C02-) and va(C02 ), associated with the M2+/carboxylate complex, and the carbonyl stretching mode v(C=0) of the proton-ated fatty acid. The disappearance of the v(C02 ) (1500-1600 cm-1) and appearance of the v(C=0) bands (—1700 cm-1), concurrent with the formation of the metal chalcogenide and regeneration of the fatty acid, have been used to evaluate... [Pg.247]


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See also in sourсe #XX -- [ Pg.21 ]




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Framework symmetric stretching modes

Stretching mode

Symmetric stretch

Symmetrical stretch

Symmetrical stretching

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