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Defect containment

First, a group of SCF-MO treated atoms which gave a physically realistic representation of quartz was determined. Following this, calculations were performed using a 3-2IG basis set on a variety of defects containing substitutionals and electron holes in quartz. [Pg.69]

The papers of Wagner and Schottky contained the first statistical treatment of defect-containing crystals. The point defects were assumed to form an ideal solution in the sense that they are supposed not to interact with each other. The equilibrium number of intrinsic point defects was found by minimizing the Gibbs free energy with respect to the numbers of defects at constant pressure, temperature, and chemical composition. The equilibrium between the crystal of a binary compound and its components was recognized to be a statistical one instead of being uniquely fixed. [Pg.3]

The observations on defect-containing crystals show that they fall broadly into two groups. In the first group the deviations from... [Pg.4]

As these questions are answered, the continuing prompt for a better understanding of why the incident occurred should be, AAdiy AAdiy did this particular occurrence occur These answers take the investigators deeper into the origin of the incident. For instance, if the oil was determined to have leaked from a defective container, one might ask ... [Pg.180]

The answer is c. Something that is defective contains a/Zflw that keeps it from working or looking as it should. [Pg.230]

The main effect of the surface treatment is the removal of the native defect containing surface on the fibers. This surface layer itself can not sustain any great degree of... [Pg.21]

One contribution is independent of the concentration of the electron defects, containing merely the chemical portion of the work to transfer one electron to infinity. We shall call this El. This term includes also the image-force effect. [Pg.230]

All real crystals have atoms which occupy external surface sites and which do not possess the correct number of nearest neighbors as a consequence, Thus, a surface is a scat of energy and is characterized by surface tension. Furthermore, internal surfaces exist, grain boundaries and twin boundaries across which atoms are incorrectly positioned. In a crystal of reasonable size—say 1 cubic centimeter, these two-dimensional defects, called surface defects, contain only about 1 atom in 106, a rather small fraction. Even so, surfaces are important attributes of solids. [Pg.1518]

Figure 8. Overall description of the acetic acid catalyzed reconstruction of a defect containing indium oxide overlayer on indium (20)... Figure 8. Overall description of the acetic acid catalyzed reconstruction of a defect containing indium oxide overlayer on indium (20)...
Alternatively, defects containing an oxygen vacancy (OV) can significantly deform the network, mainly due to mechanical distortions of the defect and its surrounding fragment. In order to simulate both network relaxation caused by the defect and its incorporation into the bulk in such systems, one needs to use larger model clusters that include at least one additional layer of bonds surrounding the defect. The atomic coordinates inside the model... [Pg.73]

Just as the oxygen vacancy and the SC can be considered as a product of the addition or disproportionation reaction of two silicon radicals (fundamental sources of the oxygen deficiency in Si02), so can the peroxide bridge and the DOSG be considered as products of the respective reactions between two oxy radicals (=Si-0-)3Si-0 (fundamental defects containing excess oxygen in silica) ... [Pg.304]

TEM examination of GaN crystals by Liliental-Weber et al [27] determined that one of the polar surfaces of high pressure solution-grown GaN crystals (especially for the smaller ones) is often atomically flat (2-3 monolayer step heights present) and that the crystal under this surface is practically free of extended defects. On the opposite surface, a number of extended defects like stacking faults, dislocation loops and Ga microprecipitates were observed. The relative thickness of the defect-containing part usually consists of 10% of the entire thickness of the platelet. [Pg.364]

Chemically-Induced Birth Defects contains information on human and other conventional mammalian teratology studies. Other kinds of reproductive toxicology are not usually covered. Full discussions are provided on chemicals for which substantial data exist, but most chemicals, for which information is much more limited, are listed in tables that summarize studies by species as + (developmental abnormalities observed), (developmental abnormalities not observed), and (equivocal results). [Pg.205]

Figure 9.1. The two-dimensional structures of a hypothetical compound J203 as, top, a crystalline solid and, bottom, a glass. The J3+ ions are shown as small shaded circles and the O2- ions as open circles. The dashed lines represent the traces of surface planes. Because of the numerous defects contained in the glass, the surface energy change corresponding to the reversible creation of a new surface is lower than that of the corresponding crystalline solid. Figure 9.1. The two-dimensional structures of a hypothetical compound J203 as, top, a crystalline solid and, bottom, a glass. The J3+ ions are shown as small shaded circles and the O2- ions as open circles. The dashed lines represent the traces of surface planes. Because of the numerous defects contained in the glass, the surface energy change corresponding to the reversible creation of a new surface is lower than that of the corresponding crystalline solid.
Negative U defects pin the Fermi energy. Since the upper le level is empty, and the lower 2e level is filled, must obviously lie between these two energy levels. The pinning of the Fermi energy position is demonstrated by assuming that the AT defects contain a variable density of electrons, n, where 0 < < IN. The law of mass action (see Section... [Pg.101]

The H-I defect contains only one 0-H bond, therefore the assirmption that its direction coincides with the induced dipole moment is firlfdled automatically. The H-II defect contains two 0-H species and according to the isotope substitution data (see bottom spectrum in Fig. I), the coupling between the two LVMs of the defect is rather weak, i. e. substitution of one hydrogen atom comprising the defect with deuterium does not change the LVM frequency of the second 0-H bond considerably. Thus, the 0-H bonds of H-II vibrate independently, and from the polarized absorption spectra we get directly the bond angles. [Pg.137]

Absorption spectra of as-grown hydrothermal ZnO samples reveal a number of lines located in the region characteristic of 0-H stretch LVMs. Based on the isotope substitution experiments as well as on the polarization studies, it is shown that at least one of these lines, at 3577.3 cm , originates from a defect containing one 0-H bond primarily aligned with the c axis of the crystal and labeled as H-I. The presence of a native defect is tentatively suggested. [Pg.143]


See other pages where Defect containment is mentioned: [Pg.224]    [Pg.326]    [Pg.1246]    [Pg.75]    [Pg.74]    [Pg.160]    [Pg.538]    [Pg.4]    [Pg.18]    [Pg.190]    [Pg.192]    [Pg.1]    [Pg.8]    [Pg.18]    [Pg.488]    [Pg.101]    [Pg.180]    [Pg.591]    [Pg.118]    [Pg.261]    [Pg.443]    [Pg.118]    [Pg.523]    [Pg.22]    [Pg.104]    [Pg.329]    [Pg.47]    [Pg.148]    [Pg.174]    [Pg.323]    [Pg.329]    [Pg.118]    [Pg.136]   
See also in sourсe #XX -- [ Pg.44 ]




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