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Ion scattering methods

Because electron-spectroscopic and ion-scattering methods yield information about the first seven atom layers, applying these techniques to metal-hydrogen kinetic problems requires incorporating depth-profiling capability. That is, an argon-sputtering gun must be incorporated into the analysis system to remove undesired surface material up to several nanometers deep. [Pg.390]

P.R. Watson. Critical Compilation of Surface Structures Determined by Ion Scattering Methods. J. Phys. Chem. Ref. Data 19 85 (1990). [Pg.32]

In tenns of individual techniques, table B1.2T1 lists tlie breakdown totalled over time, counting from the inception of surface stmctural detennination in the early 1970s. It is seen that LEED has contributed altogether about 67% of all stmctural detenninations included in the database. The annual share of LEED was 100% until 1978, and has generally remained over 50% since then. In 1979 other methods started to produce stmctural detenninations, especially PD, ion scattering (IS) and SEXAFS. XRD and then XSW started to contribute results in the period 1981-3. [Pg.1757]

In TOF-SARS [9], a low-keV, monoenergetic, mass-selected, pulsed noble gas ion beam is focused onto a sample surface. The velocity distributions of scattered and recoiled particles are measured by standard TOF methods. A chaimel electron multiplier is used to detect fast (>800 eV) neutrals and ions. This type of detector has a small acceptance solid angle. A fixed angle is used between the pulsed ion beam and detector directions with respect to the sample as shown in figure Bl.23.4. The sample has to be rotated to measure ion scattering... [Pg.1805]

Aono M, Katayama M and Nomura E 1992 Exploring surface structures by coaxial impact collision ion scattering spectroscopy (CAICISS) Nucl. Instrum. Methods B 64 29-37... [Pg.1825]

Taglauer E, Beckschulte M, Margraf R and Mehl D 1988 Recent developments in the applications of ion scattering spectroscopy Nucl. Instrum. Methods B 35 404-9... [Pg.1825]

Ion Scattering Spectroscopy (ISS) is one of the most powerful and practical methods of surface analysis available. However, it is undemtilized due to a lack of understanding about its application and capabilities. This stems from its history, the limited number of high-performance instmments manufactured, and the small number of experienced surface scientists who have actually used ISS in extensive applications. Ironically, it is one of the easiest and most convenient sur ce analytical instruments to use and it provides usehil information for almost any type of solid material. [Pg.514]

Xiang, T.-X. Anderson, B. D., Development of a combined NMR paramagnetic ion-induced line-broadening dynamic light scattering method for permeability measurements across lipid bilayer membranes, J. Pharm. Sci. 84, 1308-1315 (1995). [Pg.275]

Methods based on the study of the scattering of an ion beam also belong among techniques for analysis of surfaces that have been used only occasionally in electrochemistry. The ion-scattering spectroscopic (ISS) method studies the scattering of slow ions (with energy up to 1 keV). The... [Pg.349]

Although X-ray and neutron diffraction and scattering methods give only approximate estimates of hydration numbers they can provide precise measures of ion-water distances in solution. In calcium chloride and bromide solutions of various concentrations, Ca-0 distances of between 2.40 and 2.44 A have been reported (167,168,171,172) Ca-0 — 2.26A was claimed in an early X-ray investigation of molar calcium nitrate solution (167,186). EXAFS and LAXS studies showed a broad and asymmetric distribution of Ca-0 distances centered on a mean value of 2.46 A (174). [Pg.271]

Fig. 4 PIC dye nanoparticles prepared by the ion-association method. (1) Particle size distributions (determined by the dynamic light scattering technique) and the corresponding electron micrographs of the dye nanoparticles. The average diameter can be controlled by tuning the molar ratio of TPB- to PIC+ (=[TPB-]/[PIC+]. With an increase in the molar ratio, the average diameter decreased. (2) Absorption spectra of PIC nanoparticles in aqueous solution with different sizes (125 and 64 nm in diameter), exhibiting size-dependent peak shift of the 0-0 band. The spectrum of the aqueous PIC-Br monomer solution is also shown... Fig. 4 PIC dye nanoparticles prepared by the ion-association method. (1) Particle size distributions (determined by the dynamic light scattering technique) and the corresponding electron micrographs of the dye nanoparticles. The average diameter can be controlled by tuning the molar ratio of TPB- to PIC+ (=[TPB-]/[PIC+]. With an increase in the molar ratio, the average diameter decreased. (2) Absorption spectra of PIC nanoparticles in aqueous solution with different sizes (125 and 64 nm in diameter), exhibiting size-dependent peak shift of the 0-0 band. The spectrum of the aqueous PIC-Br monomer solution is also shown...
Surface concentrations deduced from low-energy ion scattering (LEIS) spectra analysis showed that as erosion increases with time, the concentration of palladium increases whereas that of tin decreases. This result is in agreement with a pronounced surface enrichment by tin with respect to palladium according to the principle of the preparation method. [Pg.277]

The calculated Rayleigh mode (SJ, the lowest lying phonon branch, is in good agreement with the experimental data of Harten et al. for all three metals. Due to symmetry selection rules the shear horizontal mode just below the transverse bulk band edge can not be observed by scattering methods. The mode denoted by Sg is the anomalous acoustic phonon branch discussed above. Jayanthi et al. ascribed this anomalous soft resonance to an increased Coulomb attraction at the surface, reducing the effective ion-ion repulsion of surface atoms. The Coulomb attraction term is similar for all three metals... [Pg.245]

In addition, many of the ferroelectric solids are mixed ions systems, or alloys, for which local disorder influences the properties. The effect of disorder is most pronounced in the relaxor ferroelectrics, which show glassy ferroelectric behavior with diffuse phase transition [1]. In this chapter we focus on the effect of local disorder on the ferroelectric solids including the relaxor ferroelectrics. As the means of studying the local structure and dynamics we rely mainly on neutron scattering methods coupled with the real-space pair-density function (PDF) analysis. [Pg.70]


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