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Determination of Coverages

If one takes the above discussed restrictions into account, SHG is, for media with inversion symmetry, an extremely surface-sensitive method. This class of media covers face centered cubic, fee (gold, etc.) and body centered cubic, bcc (sodium, etc.) metals, diamond, silicon, germanium, all gases and liquids or glasses. Depending on the absolute value of the components of adsorption and desorption processes might be observed in the submonolayer regime. This is demonstrated in Fig. 6.2 for CO molecules, adsorbed on Ni(lll) (Zhu et al. 1985) and in Fig. 6.3 for alkali films on Si(lll) (Bordo et al. 2005). The [Pg.144]

0i is the angle of the incoming laser beam with respect to the surface normal. For a Nd YAG laser pulse (1064 nm) of duration t = 10 ps, intensity = 10 W/cm and area f = 1 mm (corresponding to a pulse energy of 100 pj), which irradiates a monolayer of molecules with a surface susceptibility of = 10 esu, one calculates from Eq. (6.14) about 10 photons per laser pulse. In the CGS system the susceptibility is defined via The conversion factor between the two systems [Pg.145]

7) Mutual interactions of the nonlinear optically active particles modify the local fields (Ye and Shen 1983). [Pg.145]

A = 497 nm, d) T = 326 K, A = 570 nm. TTie intensity from the plain Si surface is denoted by a dashed horizontal line. Reprinted with permission from Bordo et al. (2005). Copyright 2005, EDB Sciences. [Pg.146]

Upon reflection from the surface, the local field strength tensor L has to be [Pg.146]


The absolute determination of coverage is much more difficult. The formalism is well known, i.e., it is possible to go from the intensity of a spectral ion to the concentration material on the surface, but this can only be worked out if the transition dipole moment is known. A very rough order of magnitude version of this can, however, usually be obtained by analogy (rather than by quantum mechanical calculation) so that somewhat better than an order of magnitude calculation of the coverage of the surface radicals can be given. [Pg.367]

XV. Determination of Coverage by Adsorbed H in Hydrogen Evolution Reaction at Transition Metals... [Pg.71]

Cho, B.K., Determination of coverage-dependent heat of adsorption from transient pulse experiments, Chem. Eng. Sci., 45(5), 1422-1425 (1990). [Pg.990]

Whenever the lateral interaction in an adlayer is weak, we observe a linear dependence of I R/R on coverage 6 (or on the average film thickness d). Such a relation, which simply implies that the film dielectric constants, ej, are independent of 0 (Eq. 29), is conveniently used for a precise determination of coverages and hence of adsorption isotherms. Especially in cases like halide adsorption where the evaluation of surface excesses from charge measurements is hampered by an unknown electrosorption valency (unless a very elaborate concentration dependence study is made " ), the spectroscopic method of determining coverages can indeed be advantageous. Adzic et have... [Pg.161]

Unlike Raman or infrared spectroscopy, with their well-defined capability of determining vibrational properties, the application of optical spectroscopy in the UV-visible range is less focused. This is because UV-visible reflectance spectroscopy intrinsically is to yield electronic excitation spectra, which unfortunately for solids are often broad and unstructured and hence not very informative as such. Therefore, this technique has increasingly been used for other tasks also, such as the determination of coverages, the assessment of structural information, and the study of surface roughness. The aim of this chapter was to demonstrate this versatility. [Pg.179]

Dielectric Behavior of Adsorbed Water. Determination of the dielectric absorption of adsorbed water can yield conclusions similar to those from proton NMR studies and there is a considerable, although older literature on the subject. Figure XVI-7 illustrates how the dielectric constant for adsorbed water varies with the frequency used as well as with the degree of surface coverage. A characteristic relaxation time r can be estimated... [Pg.588]

The heat of adsorption is an important experimental quantity. The heat evolution with each of successive admissions of adsorbate vapor may be measured directly by means of a calorimeter described by Beebe and co-workers [31]. Alternatively, the heat of immersion in liquid adsorbate of adsorbent having various amounts preadsorbed on it may be determined. The difference between any two values is related to the integral heat of adsorption (see Section X-3A) between the two degrees of coverage. See Refs. 32 and 33 for experimental papers in this area. [Pg.616]

Perhaps the most common use for REELS is to monitor gas—solid reactions that produce surface films at a total coverage of less than a few monolayers. When Eq is a few hundred eV, the surface sensitivity of REELS is such that over 90% of the signal originates in the topmost monolayer of the sample. A particularly powerfiil application in this case involves the determination of whether a single phase of variable composition occurs on the top layer or whether islands occur that is, whether... [Pg.327]

M. De Crescenzi. Phys. Rev. Letts. 30,1949,1987. Use of surface electron energy-loss fine structure (SEELFS) to determine oxygen-nickel bond length changes for oxygen absorbed on Ni (100) on a function of coverage from 0 to 1.0 monolayer. [Pg.334]

As with any analytical method, the ability to extract semiquantitative or quantitative information is the ultimate challenge. Generally, static SIMS is not used in this mode, but one application where static SIMS has been used successfully to provide quantitative data is in the accurate determination of the coverage of fluropolymer lubricants. These compounds provide the lubrication for Winchester-type hard disks and are direaly related to ultimate performance. If the lubricant is either too thick or too thin, catastrophic head crashes can occur. [Pg.555]

Determination of the equilibrium spreading pressure generally requires measurement and integration of the adsorption isotherm for the adhesive vapors on the adherend from zero coverage to saturation, in accord with the Gibbs adsorption equation [20] ... [Pg.9]

Eqs. (1,4,5) show that to determine the equilibrium properties of an adsorbate and also the adsorption-desorption and dissociation kinetics under quasi-equilibrium conditions we need to calculate the chemical potential as a function of coverage and temperature. We illustrate this by considering a single-component adsorbate. The case of dissociative equilibrium with both atoms and molecules present on the surface has recently been given elsewhere [11]. [Pg.444]

In addition to the temperature dependence of Sq T) is that of the correlation functions, which also determine the coverage dependence. [Pg.467]

Figure 39. Current-time variation in nickel pitting dissolution in NaCl solution.89,91 1, double-layer charging current 2, fluctuation-diffusion current 3, minimum dissolution current 4, pit-growth current (Reprinted from M. Asanuma andR. Aogaki, Nonequilibrium fluctuation theory on pitting dissolution. II. Determination of surface coverage of nickel passive film, J. Chem. Phys. 106, 9938, 1997, Fig. 2. Copyright 1997, American Institute of Physics.)... Figure 39. Current-time variation in nickel pitting dissolution in NaCl solution.89,91 1, double-layer charging current 2, fluctuation-diffusion current 3, minimum dissolution current 4, pit-growth current (Reprinted from M. Asanuma andR. Aogaki, Nonequilibrium fluctuation theory on pitting dissolution. II. Determination of surface coverage of nickel passive film, J. Chem. Phys. 106, 9938, 1997, Fig. 2. Copyright 1997, American Institute of Physics.)...
As previously noted, determination of the promotion index PI0s- of the promoting oxide ions O6 requires knowledge of the coverage of O6 on the... [Pg.200]

For liquid electrode metals (mercury, gallium) the determination of the surface tension can be applied. From changes of the surface tension as a function of dissolved adsorbable species the surface coverage... [Pg.239]

Measuring the uptake of a gas by a surface as a function of the dose to which the surface is exposed is the most straightforward way to determine a sticking coefficient. In such experiments, great care should be taken to ensure that gas and surface are in thermal equilibrium. In addition, we need to determine the coverage, either by surface sensitive methods (XPS, AES, IR) or by thermal desorption and ensure that adsorption is not accompanied by desorption. [Pg.268]

For ammonia synthesis, we still need to determine the coverages of the intermediates and the fraction of unoccupied sites. This requires a detailed knowledge of the individual equilibrium constants. Again, some of these may be accessible via experiments, while the others will have to be determined from their respective partition functions. In doing so, several partition functions will again cancel in the expressions for the coverage of intermediates. [Pg.297]

Determine the coverages of atomic hydrogen and CO for the following three gas mixtures ptot = 1 bar and pco= 1,10,100 ppm. The operational temperature of the fuel cell is 80 °C and the following information on the adsorption... [Pg.417]

The non situ experiment pioneered by Sass uses a preparation of an electrode in an ultrahigh vacuum through cryogenic coadsorption of known quantities of electrolyte species (i.e., solvent, ions, and neutral molecules) on a metal surface. " Such experiments serve as a simulation, or better, as a synthetic model of electrodes. The use of surface spectroscopic techniques makes it possible to determine the coverage and structure of a synthesized electrolyte. The interfacial potential (i.e., the electrode work function) is measured using the voltaic cell technique. Of course, there are reasonable objections to the UHV technique, such as too little water, too low a temperature, too small interfacial potentials, and lack of control of ionic activities. ... [Pg.32]


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