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Polarised atoms analysis

The adsorption site, i.e. the chemisorption position of the adatoms on (within, below) the substrate surface, thanks to the polarisation dependence of SEXAFS. Often a unique assignment can be derived from the analysis of both polarisation dependent bond lengths and relative coordination numbers. The relative, polarisation dependent, amplitudes of the EXAFS oscillations indicate without ambiguity the chemisorption position if such position is the same for all adsorbed atoms. More than one chemisorption site could be present at a time (surface defect sites or just several of the ideal surface sites). If the relative population of the chemisorption sites is of the same order of magnitude, then the analysis of the data becomes difficult, or just impossible. [Pg.98]

The quasi-ideality of the (1 x l)Co/Cu(lll) and (1 x l)Co/Cu(110) monolayer interfaces allows a temperature dependent study of the polarisation dependent Debye Waller damping of the EXAFS oscillations i.e the analysis of the amplitude of the mean square relative displacements of the Co atoms parallel to the adsorbate layer, or perpendicular to it. The results are based on the analysis of data collected with the sample temperature T = 77 K and T = 300 K. The S—S and S—B (see above)... [Pg.110]

In principle, charge transfer spectra should be full of valuable information, because they depend on the properties of two atoms, bonded together. However, they have proved to be far less amenable to detailed analysis than d-d bands, mainly because the changes in interelectron repulsion which accompany charge transfer are not so easily parameterised. Single crystal measurements, using polarised light at low temperatures, are important and valuable in the study of d-d spectra, but... [Pg.63]

The principal values of the 15N chemical shift tensors for the amine and imine nitrogen atoms were derived from analysis of 15N lineshapes recorded for static powder samples under conditions of cross polarisation and H decou-... [Pg.24]

Various theoretical models, such as the excited-atom approach [1] and the thermochemical model [2,3] have been proposed for the determination of these shil ts. A model based on the density-functional theory has been suggested and applied for the analysis of core hole screening in simple metals by Ambladh and von Barth [4] and by Williams and Lang [5]. Spin-polarised density-functional... [Pg.433]

This example is illustrated in Figure 13.9 in which the MAS spectrum (a) is represented with the spectrum obtained from cross polarisation (b). The comparison of the two clearly shows a relative increase in certain peaks these are the Si (OH) (Si)4, , n taking the values shown on the spectrum (b). The Si (OSi)4 signal is still present this is simply due to an extended contact time which permits the polarisation to be extended over 3 bonds. It may thus be necessary to vary the contact time in order to fully discriminate the atoms bearing hydroxyls, Quantitative analysis is not possible but the experiment can be used to determine the presence or absence of silanol groups. [Pg.252]

Ylides Coordinated to Metals. - The structure of a barium complex (52) of methylbenzylidenetriphenylphosphorane has been reported. The Ba ion is in contact with both the ylidic- and the benzylic-carbon atoms. Ab initio calculations and NPA charge analysis indicate that the ylidic moiety is highly polarised, P -C . [Pg.240]

The most interesting case is photoemission of 4/ electrons in the rare earths as noted in the previous section, because of the collapsed nature of the 4/ orbitals, the photoemission spectrum can be interpreted completely even in the solid by atomic multiplet theory, and this applies also to magnetic circular dichroism. Thole and van der Laan [642] have derived sum rules for magnetic dichroism in rare-earth 4/ photoemission. They have shown that the integrated intensity is simply the sum over each sublevel of its occupation number times the total transition probability from that sublevel to the continuum shell. Polarisation effects in the 4/ photoemission spectra of rare earths are very large, and this tool based on quasiatomic analysis is of considerable significance it provides a new... [Pg.425]

Decomposition of spectrum into 5 components (fig. 6) has been carried out since XRD analysis allows to identify 5 different locations of P atoms. Moreover the low intensity peak B near -23 ppm is highly enhanced by cross polarisation which is obviously due to the proximity of protons as hydroxyl groups or water molecules. XRD pattern analysis allowed us to locate water dimers within the elliptical channels as shown in fig. 7. The broad peak A at = -20 to - 23 ppm was observed to be part of the spectrum and was assigned to an amorphous AIPO4 phase. [Pg.34]

Much attention has been given to the analysis of OH stretching bands of micas occurring in an isolated region of the spectrum ranging from about 3750 to 3550 cm (Farmer 1974). Using polarized radiation, the pleochroic scheme of IR absorption bands, measured on oriented crystal sections, makes it possible to impose defined constraints on the orientation of the OH dipoles. In a fundamental polarised IR study, Tsuboi (1950) determined the position of the H atom in the structure of muscovite. The variation of absorption intensity of the OH stretching band with the direction of the electric vector of... [Pg.359]


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Atomic analyses

Polarisability

Polarisable

Polarisation

Polarisation atomic

Polarisation atoms

Polarised atoms

Polariser

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