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Spectroscopic Correspondences

On the other hand, TDS could resolve the individual process of bond breaking, i.e., the opposite process of bond forming by thermal activation [62]. TDS profiles possess peaks of which the intensities oscillate with increasing oxygen exposure. For example, TDS from O-Pd [63] and O-Rh [64] surfaces shows a similar number of peaks (4—5) with slight difference in the characteristic peak temperatures. The TDS peaks correspond to different bond strengths and the peak intensity oscillation to the bond forming kinetics. [Pg.8]

Therefore, the variation in the spectral features of STS, UPS, TDS, and EELS corresponds to the dynamics of bond formation and relaxation, bond strength, and the adsorbate-derived valence DOS relaxation. [Pg.8]


One is familiar with the idea of discrete and definite electronic stales in molecules, as revealed by molecular spectroscopy. Each electronic stale possesses a number of vibrational states that are occupied to a great extent near the ground state at normal temperatures. Each vibrational state has, if the stcric conditions are enabling, a number of rotational states associated with it, and for gas molecules both the vibrational and the rotational states can easily be observed and measured spectroscopically. Correspondingly, the distribution of the vibrational states in solids (phonon spectra) is easily measurable. [Pg.746]

There is no evidence for discrete ionic fluoroxenon. species in WFt solution. In addition to the lack of spectroscopic correspondence with the XeFJ and XeiF), cations, the following pieces of evidence may be cited to support this view (i) Compounds such as XeFJBFr are insoluble in WFj, (ii) Removal of solvent from solutions of XcFe in WFs by pumping at low temperature leaves pure xenon hexafluoride, (iii) A F-NMR study of xenon hexafluoride in WF, shows no exchange between xenon hexafluoride, solvent, and the XeOF4 impurity. [Pg.156]

A classical Hamiltonian is obtained from the spectroscopic fitting Hamiltonian by a method that has come to be known as the Heisenberg correspondence [46], because it is closely related to the teclmiques used by Heisenberg in fabricating the fomi of quantum mechanics known as matrix mechanics. [Pg.68]

The question of non-classical manifestations is particularly important in view of the chaos that we have seen is present in the classical dynamics of a multimode system, such as a polyatomic molecule, with more than one resonance coupling. Chaotic classical dynamics is expected to introduce its own peculiarities into quantum spectra [29, 77]. In Fl20, we noted that chaotic regions of phase space are readily seen in the classical dynamics corresponding to the spectroscopic Flamiltonian. Flow important are the effects of chaos in the observed spectrum, and in the wavefiinctions of tire molecule In FI2O, there were some states whose wavefiinctions appeared very disordered, in the region of the... [Pg.76]

As in classical mechanics, the outcome of time-dependent quantum dynamics and, in particular, the occurrence of IVR in polyatomic molecules, depends both on the Flamiltonian and the initial conditions, i.e. the initial quantum mechanical state I /(tQ)). We focus here on the time-dependent aspects of IVR, and in this case such initial conditions always correspond to the preparation, at a time of superposition states of molecular (spectroscopic) eigenstates involving at least two distinct vibrational energy levels. Strictly, IVR occurs if these levels involve at least two distinct... [Pg.1058]

Figure Bl.22.11. Near-field scanning optical microscopy fluorescence image of oxazine molecules dispersed on a PMMA film surface. Each protuberance in this three-dimensional plot corresponds to the detection of a single molecule, the different intensities of those features being due to different orientations of the molecules. Sub-diffraction resolution, in this case on the order of a fraction of a micron, can be achieved by the near-field scaiming arrangement. Spectroscopic characterization of each molecule is also possible. (Reprinted with pennission from [82]. Copyright 1996 American Chemical Society.)... Figure Bl.22.11. Near-field scanning optical microscopy fluorescence image of oxazine molecules dispersed on a PMMA film surface. Each protuberance in this three-dimensional plot corresponds to the detection of a single molecule, the different intensities of those features being due to different orientations of the molecules. Sub-diffraction resolution, in this case on the order of a fraction of a micron, can be achieved by the near-field scaiming arrangement. Spectroscopic characterization of each molecule is also possible. (Reprinted with pennission from [82]. Copyright 1996 American Chemical Society.)...
The pyrolysis of CR NH (<1 mbar) was perfomied at 1.3 atm in Ar, spectroscopically monitoring the concentration of NH2 radicals behind the reflected shock wave as a fiinction of time. The interesting aspect of this experiment was the combination of a shock-tube experiment with the particularly sensitive detection of the NH2 radicals by frequency-modulated, laser-absorption spectroscopy [ ]. Compared with conventional narrow-bandwidth laser-absorption detection the signal-to-noise ratio could be increased by a factor of 20, with correspondingly more accurate values for the rate constant k T). [Pg.2125]

Similar degradation reactions were used to estabUsh the absolute configuration of mocimycin (kirromycin) (1, R = H) (46), the constitution of which had been described previously (7,47). The chemical stmctures of most other subsequentiy discovered elfamycins have been deterrnined spectroscopically and assignments of absolute configurations are not complete. The elfamycin stmctures shown in Figure 1 have complete stereochemical details that have been in part ascertained experimentally and in part are assumed to correspond to the aurodox topography. [Pg.524]

Figure 8 Spectroscopic study of GaAs(110). With a positive voltage on the STM tip, the left-hand image represents As atoms, while the corresponding negative tip voltage on the right shows Ga atoms. (Courtesy of Y. Yang and J.H. Weaver, University of Minnesota)... Figure 8 Spectroscopic study of GaAs(110). With a positive voltage on the STM tip, the left-hand image represents As atoms, while the corresponding negative tip voltage on the right shows Ga atoms. (Courtesy of Y. Yang and J.H. Weaver, University of Minnesota)...
SALI compares fiivorably with other major surface analytical techniques in terms of sensitivity and spatial resolution. Its major advantj e is the combination of analytical versatility, ease of quantification, and sensitivity. Table 1 compares the analytical characteristics of SALI to four major surfiice spectroscopic techniques.These techniques can also be categorized by the chemical information they provide. Both SALI and SIMS (static mode only) can provide molecular fingerprint information via mass spectra that give mass peaks corresponding to structural units of the molecule, while XPS provides only short-range chemical information. XPS and static SIMS are often used to complement each other since XPS chemical speciation information is semiquantitative however, SALI molecular information can potentially be quantified direedy without correlation with another surface spectroscopic technique. AES and Rutherford Backscattering (RBS) provide primarily elemental information, and therefore yield litde structural informadon. The common detection limit refers to the sensitivity for nearly all elements that these techniques enjoy. [Pg.560]

In addition to qualitative analysis of nearly all the elements of the periodic table, EEL spectra also enable determination of the concentration of a single element which is part of the transmitted volume and hence gives rise to a corresponding ionization edge. As in all comparable spectroscopic techniques, for quantification the net edge signal, which is related to the number N of excited atoms, must be extracted from the raw data measured. The net intensity 4 of the feth ionization shell of an individual element is directly connected to this number, N, multiplied by the partial cross-section of ionization ) and the intensity Iq of the incident electron beam, i.e. ... [Pg.65]


See other pages where Spectroscopic Correspondences is mentioned: [Pg.40]    [Pg.8]    [Pg.40]    [Pg.8]    [Pg.79]    [Pg.712]    [Pg.12]    [Pg.15]    [Pg.66]    [Pg.76]    [Pg.200]    [Pg.1060]    [Pg.1063]    [Pg.1716]    [Pg.1973]    [Pg.2114]    [Pg.2144]    [Pg.530]    [Pg.568]    [Pg.250]    [Pg.251]    [Pg.534]    [Pg.307]    [Pg.113]    [Pg.257]    [Pg.302]    [Pg.307]    [Pg.216]    [Pg.272]    [Pg.493]    [Pg.248]    [Pg.276]    [Pg.6]    [Pg.6]    [Pg.97]    [Pg.120]    [Pg.88]    [Pg.9]    [Pg.42]    [Pg.194]    [Pg.249]   


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