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Vibrational shift

Figure 11. Infrared resonance enhanced photodissociation spectrum of V (OCO)5 obtained by monitoring loss of CO2. The antisymmetric stretch of outer-shell CO2 is near 2349 cm (the value in free CO2, indicated by the dashed vertical line). The vibration shifts to 2375 cm for inner-shell CO2. Figure 11. Infrared resonance enhanced photodissociation spectrum of V (OCO)5 obtained by monitoring loss of CO2. The antisymmetric stretch of outer-shell CO2 is near 2349 cm (the value in free CO2, indicated by the dashed vertical line). The vibration shifts to 2375 cm for inner-shell CO2.
The molecular natures of salts crystallized from salbutamol base have been assessed by FT-Raman spectroscopy [66]. Variations in vibrational frequencies due to electron-withdrawing or -donating substituents were clearly evident the CCO stretching vibration shifted from 776 cm-1 in the free base to 756 cm-1 in the benzoate salt. The C=C stretching frequency also shifted from 1610 cm-1 to 1603 cm-1 with the benzoate ion but showed an increase to 1616 cm-1 with sulfate ion. Clearly, the choice of salt affects the molecular nature of the drug, with obvious implications for its physicochemical properties. [Pg.88]

While the BC configuration for the B—H complex is now accepted, several aspects of the vibrational spectra of the acceptor-H complexes are not understood. The temperature dependence of the B—H complex has been examined by Raman spectroscopy (Stutzmann and Herrero, 1987) and IR absorption (Stavola et al., 1988a). The H-stretching vibration shifts from 1875 to 1903 cm 1 between room temperature and liquid He temperature. Frequency shifts of just a few cm 1 are more typical for local vibrational modes. The vibrational bands are also surprisingly broad. [Pg.162]

TPD and EELS experiments have shown coadsorbed NO/NH3 to form a surface stabilized complex on Pt(lll). This assertion was based in part on the very large vibrational shifts observed for the neat (NO or NH3) systems compared to the mixed system, and in part on the simultaneous desorption of NO and NH3 from the mixed system at values of Tg higher than typical of desorption from the neat systems at comparable initial coverage Kinetit y, desorption from this system has been characterized as reaction limited,... [Pg.55]

Fig. 7.1 Infrared spectra of iron oxides in the range 400 to 4000 cm (ca. 1 mg in 300 mg KBr). a) Wave number range 1000-4000 cm b) wave number range 400-1000 cm The insert in the goethite spectrum shows that the two OH bending vibrations shift to higher wave... Fig. 7.1 Infrared spectra of iron oxides in the range 400 to 4000 cm (ca. 1 mg in 300 mg KBr). a) Wave number range 1000-4000 cm b) wave number range 400-1000 cm The insert in the goethite spectrum shows that the two OH bending vibrations shift to higher wave...
The band shift model of Gillis-D Hamers7 is based on the observation that the peak maximum of the free silanol vibration shifts as a function of treatment temperature (figures 5.6 and 5.7). Measurements were performed using the FTIR technique, in the high resolution (0.5 cm 1) mode. [Pg.99]

The physical interaction between =sSi-NH2 and NH4C1 is reflected in the N-H stretching region of the amine functions. When the temperature is raised, the symmetrical Si-NH2 band shifts from 3505 cm 1 to 3530 cm 1 and the asymmetrical vibration shifts from 3430 cm 1 to 3450 cm1. Van Der Voort has shown that the peak shift is a discrete function of temperature (figure 12.9). [Pg.398]

The 0-H stretching and N-H stretching bands form the broad band between 3500 and 3200 cm-. Infrared bands associated with the 0-H and N-H stretching vibrations shift towards higher wavenumbers as the hydrogen bond decreases in energy and is eventually lost. [Pg.251]

In this chapter we summarize our present knowledge of chemical compounds that contain positrons or positronium. We do not give an exhaustive review of the literature, but rather we try to give information that is correct up to at least January 1, 2002. Since most of our knowledge of bound positronic systems comes from theoretical work, this chapter is primarily concerned with quantum mechanics. The most conspicuous exception is provided by recent observations of vibrational shifts of compounds that have resonantly captured a positron [l], implying the existence of bound states. [Pg.17]

Figure 3. The different contribution to the Hartree-Fock vibrational shift of chemisorbed CO. FO stands for the Pauli repulsion or Frozen Orbital, FO, contribution, "pol Pt " and "don Pt " correspond to the substrate polarization and donation from the subtrate to the CO adsorbed molecule (ji-backdonation), "pol CO" and "don CO" stand for to the CO polarization and donation from CO to the surface (o-donation), SCF contains the rest of contributions due to coupling between the different mechanisms. Figure 3. The different contribution to the Hartree-Fock vibrational shift of chemisorbed CO. FO stands for the Pauli repulsion or Frozen Orbital, FO, contribution, "pol Pt " and "don Pt " correspond to the substrate polarization and donation from the subtrate to the CO adsorbed molecule (ji-backdonation), "pol CO" and "don CO" stand for to the CO polarization and donation from CO to the surface (o-donation), SCF contains the rest of contributions due to coupling between the different mechanisms.
Dehydro- -Cyclocitrylideneacetic Acid (49). In order to determine the influence of a supplementary double bond in the cycle of 3-ionone on the proposed mechanism, we were interested in the irradiation of compounds of the dehydro- 3-ionone series. Dehydro- 8-cyclocitrylidene-acetic acid (49), prepared from- -cyclocitiyhdeneacetic acid according to the method of Henbest used by him to obtain dehydro- 3-ionone) has been irradiated in hexane. The conjugation bands 1610-1630 cm. and CH=CH trans absorption at 960 cm. characteristic of 49, disappeared and were replaced by a methenic band at 895, cm. the carbonyl vibration shifted from 1695 to 1705 cm. The UV absorption at 320 mitt disappeared while maxima at 200, 235, and 270 my appeared. [Pg.208]

This apparent contradiction has stimulated a considerable amount of theoretical work from the early 90 s until very recently. A number of more and more refined calculations has been performed by several groups using various methods [72], from simple HF [73,74] to HF with extended inclusion of correlation [75,76], from LDA [77] to gradient corrected DFT [78,79]. However, the most sophisticated methods and calculations lead to the same conclusion CO is bound to the terrace sites of the MgO surface through electrostatic forces, with a very weak binding energy of less then 0.1 eV, and a very small vibrational shift, of -I-IO cm" or less [67,72]. Eventually, the discrepancy between the ab initio calculations and the results on MgO thin films lead to the suggestion that surface defects could be responsible for the observed chemisorption properties of CO/MgO/Mo(l 10). [Pg.104]

In the field of catalysts characterization the use of small unreactive probe molecules to identify coordinatively unsaturated sites is well established [89]. Not always, however, a direct correlation between the CO vibrational frequency, the strength of the interaction, and the surface electric field exists. Recent DPT cluster calculations [90] have shown that CO adsorbed on step sites gives rise to a relatively strong interaction but to a negligible CO vibrational shift this is due to the inhomogeneity in the electric field above a MgO(lOO) step. This study [90] has permitted the complete attribution of the IR spectrum of CO adsorbed on MgO [81,83,91], Table 2. [Pg.106]


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See also in sourсe #XX -- [ Pg.160 ]

See also in sourсe #XX -- [ Pg.81 , Pg.98 ]

See also in sourсe #XX -- [ Pg.81 , Pg.98 ]




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Vibration frequency shift

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Vibrational mode shifts

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