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Relaxation inward

The surface properties of metals are such that the surface tends to relax inwards bu systems described by two-body interactions tend to relax outwards. [Pg.259]

Surfaces of real crystals never adopt the bulk-truncated structures shown in Fig. 4.5. They reconstruct or relax (inwards or outward movement of the atoms) to minimize their surface energy [42]. Known surface structures of zincblende and wurtzite structure semiconductors are summarized in [43]. Nonpolar surfaces of wurtzite (1120) and (1010) surfaces show no lateral surface reconstructions and are supposed to have a structure similar to the well-known zincblende (110) surface, which is characterized by an inward relaxation of the surface cations and partial electron transfer from the surface cation dangling bond to the surface anion dangling bond [42,43]. [Pg.132]

The oscillatory behaviour of surface relaxation — inward for Af/12, outward for A 23 — seems to be fairly universal (Fu et al., 1984 Landman et al., 1980 Jiang et al., 1986). It is found not only experimentally and in fully self-consistent calculations, but also in simplified calculations a la Heine-Finnis. If a frozen charge density is used, for example a step density or the Lang -Kohn jellium surface profile, and the ions are relaxed to positions of zero force, oscillatory relaxations are found (Landman et al., 1980). This shows that it is not a consequence of the Fricdel oscillations in the surface charge density. [Pg.92]

An alternative 2 x 1 reconstruction on (100) surfaces may be obtained by removing all of the surface atoms in Fig. 10-7,a this is shown in Fig. 10-7,b. Again, the number of broken bonds is not changed but now two atoms with single dangling hybrids are present for each atom with double dangling hybrids, and the reconstruction differs. Each of these single hybrids has [111] orientation (in this case [TTT] or [1 IT]) and they will alternately relax inward and outward as on the... [Pg.440]

Low energy electron diffraction (LEED)-surface crystallography studies clearly indicate that the surfaces of most clean metals relax inward. The rougher the surface (the more open the surface structure), the greater is the relaxation. The (Iff) and (211) iron surface structures as determined by LEED-surface crystallography are shown in Fig. 3.84. d90... [Pg.292]

Atoms at the pure metal surfaces relax inwardly and reconstruct in the surface planes because of the spontaneous bond contraction and the derived tensile stress. The stress-induced inward relaxation is quite common despite the discrepancy in... [Pg.489]

Figure 7.23 A schematic diagram showing the relaxation of an island on a substrate in which the island was stretched (tensile stress) to fit the substrate lattice. To accommodate part of the lattice mismatch it relaxes inward toward the upper part of the island. Figure 7.23 A schematic diagram showing the relaxation of an island on a substrate in which the island was stretched (tensile stress) to fit the substrate lattice. To accommodate part of the lattice mismatch it relaxes inward toward the upper part of the island.
Most metal surfaces have the same atomic structure as in the bulk, except that the interlayer spaciugs of the outenuost few atomic layers differ from the bulk values. In other words, entire atomic layers are shifted as a whole in a direction perpendicular to the surface. This is called relaxation, and it can be either inward or outward. Relaxation is usually reported as a percentage of the value of the bulk interlayer spacing. Relaxation does not affect the two-dimensional surface unit cell synuuetry, so surfaces that are purely relaxed have (1 x 1) synuuetry. [Pg.288]

Kotlikoff I would agree, although we don t know what the functional effect of the release is, whether it is relaxation or contraction. One difference here is the prominent presence of inward currents that are depolarizing. [Pg.122]

Henceforth we take the primitive path co-ordinate s=L-z from the free end inwards to the branch point so that t(s) is an increasing function of s. The prefactor Tq is an inverse attempt frequency for explorations of the potential by the free end, and may be expected to scale as the Rouse time for the star arm (in fact this is not quite true - the actual scaling is as [25,26]). The relaxation mod-... [Pg.215]

Nifedipine is a calcium-channel blocker of the dihydropyridine group. It relaxes smooth muscle and dilates both coronary and peripheral arteries by interfering with the inward displacement of calcium-channel ions through the active cell membrane. Unlike verapamil, nifedipine can be given with beta-blockers. Long-acting formulations of nifedipine are preferred in the long-term treatment of hypertension. [Pg.27]

On the other hand, if a chemical is somewhat less similar to acetylcholine, it may interact with the receptor but be unable to induce the exact molecular change necessary to allow the inward movement of sodium. In this instance the chemical does not cause contraction, but because it occupies the receptor site, it prevents the interaction of acetylcholine with its receptor. Such a drug is termed an antagonist. An example of such a compound is d-tubocurarine, an antagonist of acetylcholine at the end-plate receptors. Since it competes with acetylcholine for its receptor and prevents acetylcholine from producing its characteristic effects, administration of d-tubocurarine results in muscle relaxation by interfering with acetylcholine s ability to induce and maintain the contractile state of the muscle cells. [Pg.11]

Andersson, D. A., Zygmunt, P. M., Movahed, P., Andersson, T. L., and Hogestatt, E. D. 2000. Effects of inhibitors of small- and intermediate-conductance calcium-activated potassium channels, inwardly-rectifying potassium channels and Na(+)/K(+) ATPase on EDHF relaxations in the rat hepatic artery. Br. J. Pharmacol. 129 1490-1496. [Pg.371]

For (2116) faces, the frequencies and electric fields critically depend on the relaxation because the Cr3+ ions located in exposed positions undergo a remarkable inward relaxation. [Pg.345]

Therefore, CO adsorbed on Cr3+ centers located on the (111) faces is expected to be characterized by somewhat higher frequencies. However, it has been shown for the (0001) face of a-Cr203 (where Cr3+ is in a very similar environment) that Cr3+ moves inward to a more shielded position upon relaxation, which leads to a reduced electric field strength at the chromium centers. Because of the stability of the surface complexes even at room temperature, it is not excluded that n backdonation may also play a role in the bond between the CO and the Cr3+ centers (which usually shift the CO frequency downwards). As discussed previously (see Section IV.A.4) the shift A v induced by increasing CO coverage is caused by lateral... [Pg.357]


See other pages where Relaxation inward is mentioned: [Pg.241]    [Pg.407]    [Pg.364]    [Pg.50]    [Pg.211]    [Pg.612]    [Pg.24]    [Pg.29]    [Pg.179]    [Pg.363]    [Pg.509]    [Pg.214]    [Pg.117]    [Pg.153]    [Pg.333]    [Pg.241]    [Pg.407]    [Pg.364]    [Pg.50]    [Pg.211]    [Pg.612]    [Pg.24]    [Pg.29]    [Pg.179]    [Pg.363]    [Pg.509]    [Pg.214]    [Pg.117]    [Pg.153]    [Pg.333]    [Pg.77]    [Pg.279]    [Pg.26]    [Pg.122]    [Pg.198]    [Pg.243]    [Pg.717]    [Pg.53]    [Pg.249]    [Pg.227]    [Pg.166]    [Pg.264]    [Pg.118]    [Pg.697]    [Pg.412]    [Pg.57]    [Pg.451]    [Pg.457]    [Pg.129]    [Pg.168]   
See also in sourсe #XX -- [ Pg.14 ]




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