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Crystalline surface states

All of the experiments in pure and mixed SSME systems, as well as in the Af-stearoyltyrosine systems, have one common feature, which seems characteristic of chiral molecular recognition in enantiomeric systems and their mixtures enantiomeric discrimination as reflected by monolayer dynamic and equilibrium properties has only been detected when either the racemic or enantiomeric systems have reverted to a tightly packed, presumably quasi-crystalline surface state. Thus far it has not been possible to detect clear enantiomeric discrimination in any fluid or gaseous monolayer state. [Pg.98]

Unlike ion-selective electrodes using glass membranes, crystalline solid-state ion-selective electrodes do not need to be conditioned before use and may be stored dry. The surface of the electrode is subject to poisoning, as described earlier for a Ck ISE in contact with an excessive concentration of Br. When this happens, the electrode can be returned to its original condition by sanding and polishing the crystalline membrane. [Pg.482]

Concurrent stream of the development of nanomaterials for solid-state hydrogen storage comes from century-old studies of porous materials for absorption of gasses, among them porous carbon phases, better known as activated carbon. Absorption of gases in those materials follows different principles from just discussed absorption in metals. Instead of chemisorption of gas into the crystalline structure of metals, it undergoes physisorption on crystalline surfaces and in the porous structure formed by crystals. The gases have also been known to be phy-sisorbed on fine carbon fibers. [Pg.23]

At crystalline surfaces, there are three types of wavefunctions as shown in Fig. 4.1. (1) The Bloch states are terminated by the surface, which become evanescent into the vacuum but remain periodic inside the bulk. (2) New states created at the surfaces in the energy gaps of bulk states, which decay both into the vacuum and into the bulk, the so-called surface states. (3) Bloch states in the bulk can combine with surface states to form surface re.sonances, which have a large amplitude near the surface and a small amplitude in the bulk as a Bloch wave. [Pg.91]

Such a decomposition has physical meanings in surface science. For example, the potential between an atom and a crystalline surface can be calculated as the sum of pairwise potentials the tunneling current from a tip state to a crystalline surface can be calculated as the sum of the tunneling currents to the... [Pg.354]

It is quite natural that the thermodynamic approach does not allow photocorrosion processes to be described comprehensively. In a number of cases, kinetic peculiarities of reactions play an important role (see, for example, Bard and Wrighton, 1977) these peculiarities are caused by the effect of crystalline structure, state of the semiconductor surface, etc. A detailed description of a complicated reaction with several particles in the solution and crystal lattice involved usually encounters considerable difficulties. Therefore, at this stage the kinetic approach is used to reveal purely qualitative regularities of corrosion processes. [Pg.292]

We explain the low surface recombination velocity by the sweeping of surface states from the region between the edges of the conduction and valence bands upon oxidation of the surface. The standard free energies of formation of crystalline and fused quartz from bulk Si are -192 and -191 Kcal/mole respectively. The standard free energy change for a Si surface is likely to be... [Pg.61]

The magnitude of the errors in determining the flat-band potential by capacitance-voltage techniques can be sizable because (a) trace amounts of corrosion products may be adsorbed on the surface, (b) ideal polarizability may not be achieved with regard to electrolyte decomposition processes, (c) surface states arising from chemical interactions between the electrolyte and semiconductor can distort the C-V data, and (d) crystalline inhomogeneity, defects, or bulk substrate effects may be manifested at the solid electrode causing frequency dispersion effects. In the next section, it will be shown that the equivalent parallel conductance technique enables more discriminatory and precise analyses of the interphasial electrical properties. [Pg.351]

Concerning ices, it has been discussed that they must be amorphous (Smoluchowski 1983) in the interstellar medium and not crystalline. This implies that the adsorbed H atoms are localized in deep traps so that their wavefunctions have a limited spatial extent. This fact reduces significantly their mobility and hence the interaction with another H atom absorbed on another site is slow as compared to the residence time unless the two atoms happens to be localized near each other. This phenomenon reduces the rate of H2 formation by several orders of magnitude when compared to the situation on crystalline surfaces. Computational simulations on soft and hard ice model surfaces have shown that for a cross-section of 4,000 nm2 the reaction probability is 1 (Takahashi et al. 1999). Furthermore, the H2 formed, due to the high amount of energy liberated is rapidly desorbed in an excited state from the ice mantle in timescales of 500 fs (Takahashi et al. 1999). [Pg.42]

Mineral grinding leads to distorsion of chemical and ionic bonds between atoms and ions. In the fracture areas binding and coordination states get asymmetric, and new electron and electric valences occur. Spontaneous reactions in the crystalline structure and with contact phases are the consequence of the distorsion. Surface distorsion of the crystalline structure may be diminished or completely abolished. At the same time, the free surface energy decreases due to polarization of surface ions. These ions are redistributed in the inner or outer layer of the crystalline surface and/or due to chemisorption of molecules and ions1. All these changes occur side by side, but one of them can suppress the effect of the others in a decisive manner. [Pg.93]

Lattice defects can function both as donors and as acceptors and create free electrons or electron holes. Crystalline surfaces containing unsaturated electron valences act as electron traps and capture free electrons. This leads to changes in binding conditions and in the charge state of e.g. metal ions their ability to polarize O- in a metal oxide decreases. Surface oxidation during the grinding process often causes deep alterations of the surface structure of solids (sulphides, graphite, coal). This usually leads to increases in affinity toward water and in reactivity with the surfactant. [Pg.93]

The interplay between lateral forces and interaction with the substrate is illustrated in Fig. 1. The adsorption energy Aof a single atom or molecule is modulated laterally due to the atomic corrugation of the crystalline surface. At low temperatures, the molecule will be in its ground state and immobile. In order to migrate on the surface, the molecule must overcome the acti-... [Pg.211]

B. Fubini, I. Fenoglio, Z. Elias, and O. Poirot, On the Variability of the Biological Responses to Silicas Effect of Origin, Crystallinity and State of the Surface on the Generation of Reactive Oxygen Species and Consequent Morphological Transformations in Cells, J. Environ. Pathol. Toxicol. Oncol. 20, 87-100 (2001). [Pg.252]


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See also in sourсe #XX -- [ Pg.63 , Pg.65 ]

See also in sourсe #XX -- [ Pg.63 , Pg.65 ]




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Crystalline state

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Crystalline surfaces

Surface crystallinity

Surface states

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