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Surfaces and defects

Crystalline dcfcci.s, such as vacancies, also produce dangling hybrids, and the. same kind of Jahn-Tcllcr distortion is known to occur this always tends to sweep states from the gap. The extreme case is the amorphous covalent solid, which, even though disordered, retains an open covalent structure and is semiconducting. [Pg.229]

Reconstruction, as well as other effects, shifts the absolute energies of the electrons [Pg.229]

8 cV for all polar semiconductors, and slightly more for homopolar ones. Thus, with this correction, (he absolute energies arc meaningful and can be used to estimate holerojunction band steps. [Pg.230]

Up to thi.s point we have focused almost entirely on the bulk properties of covalent crystals. Any real crystal has surfaces, but for large systems, say 10 atoms long, there are of the order of 10 atoms within the interior and only some 10 on the surface, so that many properties arc dominated by the interior. On the other hand, processes such as electron diffraction or catalysis are dominated by surface effects, and it is important that we include some discussion of them. As with other topics, this will necessarily be a cursory view, indicating some central concepts. There is a regular journal, Surface Science, exclusively devoted to current developments in the subject. We shall also discuss briefly in this chapter some related concepts concerning crystalline defects and amorphous solids. [Pg.230]

The minimizations reveal dramatic atomic relaxations accompanying a large reduction in surface energy from that given by a perfect termination of the bulk structure. As Table 11.2 makes clear, interatomic distances in the outermost layers can change by over 50% relative to the bulk values  [Pg.371]

Surface relaxation thus has several effects. It modifies and reconstructs the surface atomic structure. Surface energies are reduced (possibly by as much as a factor of three in the above example - from 6.0 to 2.0 J m-2). More generally, it can reorder the relative stability of different surfaces and thus have a profound effect on the crystal morphology. [Pg.371]

Considerable attention has also been paid to modelling the thermodynamics of defects. This includes, for example, studies of the enthalpies of formation of vacancies or interstitial atoms and the association energies associated with the clustering of such defects. It is usually crucial to allow for the relaxation of the [Pg.371]

Layer Energy minimization (using interatomic potentials) [23] ab initio (DFT) [24] Experiment [25] [Pg.371]


Wang L S, Nicholas J B, Dupuis M, Wu FI and Colson S D 1997 SijO (x = 1-6) models for oxidation of silicon surfaces and defect sites in bulk oxide materials Phys. Rev. Lett. 78 4450... [Pg.2407]

J.S. Anderson, in M.W. Roberts and J.M. Thomas (Eds.), Surface and Defect Properties of Solids, Specialist Periodical Reports, Chemical Society, London, 1972, Vol. l,p. 1. [Pg.304]

Conesa373 modeled the surfaces and defects on ceria, and based on computer simulations, determined the relative stabilities of surfaces (111) > (110) > (211) > (100). Although the formation of anion vacancy defects was suggested to be more difficult to form on the more stable (111) surface, he indicated that anion vacancy pairs, important for 02 uptake and release processes, were easiest to form on the ceria (111) surface. [Pg.224]

In summary, these experiments demonstrate that Ba2 partitioning does not depend on the concentration of Ba2 over the broad range tested and that it is unaffected by moderate amounts of Sr2. Substantial quantities of NaCl decrease kcBa and rapid precipitation increases kcBa. These results suggest little or none of the Ba2 is incorporated in Ca 2 lattice sites in calcite, but instead adsorbs on surfaces and defects and is trapped by growth of the crystal. [Pg.583]

Ross, J. R. H. In Surface and Defect Properties of Solids, Roberts,... [Pg.549]

Anderson, J. S. (1972a) in Surface and Defect Properties of Solids (eds Roberts, M. W. Thomas, J. M.) Vol. 1, The Chemical Society, London. [Pg.277]

R. Kellerman and K. Klier, Surface and Defect Properties in Solids, Chem, Soc. London,... [Pg.242]

AndersonJ S, Surface and defect properties of solids, Vol. 1, edited... [Pg.56]

Molecular Structure by Diffraction Methods Vol. 6 Senior Reporters Prof. M. R. TRUTER and Dr. L. E. SUTTON Hardcover 348 pp 0 85186 557 7 Chemical Physics of Solids and their Surfaces Vol. 8 (successor to "Surface and Defect Properties of Solids") Senior Reporters Prof. M. W. ROBERTS and Prof. J. M. THOMAS Hardcover 260 pp 0 85186 740 5... [Pg.180]

There are other methods of NDI other than X-ray radiography. One of them is ultrasonic NDI. In this technique, ultrasonic waves are used to investigate the interior of a ceramic piece. An ultrasonic transducer placed on the surface of the ceramic piece sends the ultrasonic waves received by a sensor found either within the ultrasonic transducer or at another location on the surface of the ceramic piece. Ultrasonic waves are scattered emd reflected back finm the surfaces and defects within... [Pg.886]


See other pages where Surfaces and defects is mentioned: [Pg.2913]    [Pg.259]    [Pg.395]    [Pg.33]    [Pg.33]    [Pg.305]    [Pg.28]    [Pg.156]    [Pg.54]    [Pg.54]    [Pg.370]    [Pg.86]    [Pg.89]    [Pg.277]    [Pg.278]    [Pg.160]    [Pg.120]    [Pg.270]    [Pg.186]    [Pg.317]    [Pg.160]    [Pg.140]    [Pg.238]    [Pg.2]    [Pg.198]    [Pg.33]    [Pg.33]    [Pg.80]    [Pg.269]    [Pg.433]    [Pg.164]    [Pg.270]    [Pg.433]    [Pg.301]    [Pg.229]    [Pg.230]   


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