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Silicon structure

A useful notation and abbreviation of the complex silicone structures takes advantage of the number of oxygen atoms around the silicon atom in a siloxy unit [1]. This notation uses the letters M, D, T and Q to represent siloxy units where the silicon atom is linked with one, two, three or four oxygen atoms, respectively (Scheme 1). Fractions are used in this notation to take into account an equal share of an oxygen atom with adjacent siloxy monomeric units. [Pg.678]

Fig. 6. Coordination geometry at silicon structures of the complexes 4 (left) and 5 (right)... Fig. 6. Coordination geometry at silicon structures of the complexes 4 (left) and 5 (right)...
FIGURE 14.42 A typical silicone structure. The hydroc arbon groups give the substance a water-repelling quality. Note the similarity of this structure to that of the purely inorganic pyroxenes in Fig. 14.38. [Pg.734]

The interaction between particle and surface and the interaction among atoms in the particle are modeled by the Leimard-Jones potential [26]. The parameters of the Leimard-Jones potential are set as follows pp = 0.86 eV, o-pp =2.27 A, eps = 0.43 eV, o-ps=3.0 A. The Tersoff potential [27], a classical model capable of describing a wide range of silicon structure, is employed for the interaction between silicon atoms of the surface. The particle prepared by annealing simulation from 5,000 K to 50 K, is composed of 864 atoms with cohesive energy of 5.77 eV/atom and diameter of 24 A. The silicon surface consists of 45,760 silicon atoms. The crystal orientations of [ 100], [010], [001 ] are set asx,y,z coordinate axes, respectively. So there are 40 atom layers in the z direction with a thickness of 54.3 A. Before collision, the whole system undergoes a relaxation of 5,000 fsat300 K. [Pg.240]

In the case of neutral systems the geometry corresponds to a bicapped tetrahedron or, in other words, to a tetrahedron which undergoes two nucleophilic coordinations. They have been observed [5] to be stable in solution. A careful H variable temperature NMR study shows that these compounds undergo an intramolecular isomerization which takes place without cleavage of Si-N bonds. The AGt of this so-called "Baylar Twist" isomerization has been estimated at between 12 and 18 kcal/mole depending on the substituents at the silicon. We can conclude that this work supports strongly hexacoordinated silicon structures as possible intermediates in the usual course of nucleophilic reactions at silicon. [Pg.158]

QC in silicon structures requires dimensions of a few nanometers and is therefore proposed to be responsible for the formation of microporous films on Si electrodes, as discussed in Chapter 7. QC is independent of doping and is often found as a superposition to pore formation by SCR effects. Only for p-type silicon electrodes of doping densities of 1016-1017 cm-3 is no formation of SCR-related pores observed upon anodization in aqueous HF. This substrate doping regime is therefore best suited for formation of purely microporous layers. [Pg.103]

This section gives a brief overview of theoretical investigations dealing with the properties of quantum-confined silicon structures. [Pg.150]

Silicon microstructures can be categorized according to the dimensionality of the confinement. Most PL studies deal with silicon structures confined in three dimensions such dot-like structures are designated zero-dimensional (OD). An overview of size-dependent properties of silicon spheres is given in Table 6.1. Standard methods of generating such microstructures are gas-phase synthesis [Di3, Li7, Scl2], plasma CVD [Ru2, Col, Ta8] or conventional chemical synthesis [Mal5]. [Pg.165]

G. Sberveglieri. Thin-film gas sensor implemented on a low-power-consumption mi-cromachined silicon structure . Sensors and Actuators B49 (1998), 88-92. [Pg.115]

D. Modroukas, V. Modi, and L. G. Chette. Micromachined silicon structures for free-convection PEM fuel cells. Journal of Micromechanics and Microengineering 15 (2005) S193-S201. [Pg.291]

Figure 1. Silicone structure consists of Si—O—Si backbone that provides thermal stability of the material. Hydrocarbon radicals that attach to silicon atoms provide water-repelling properties. Figure 1. Silicone structure consists of Si—O—Si backbone that provides thermal stability of the material. Hydrocarbon radicals that attach to silicon atoms provide water-repelling properties.
Silicone acrylates Acrylated organopolysiloxanes exhibit excellent release properhes and are used as release coahngs on papers and films. The silicone structure provides flexibility and resistance to heat, moisture, radiahon degradahon, and shear forces. ... [Pg.76]

The additional symmetry elements in the silicon structure are given in Table 17.12. At A, P(k) C4V, which is isomorphous with Gg. Jones symbols and the character table are in Table 17.15. [Pg.382]

D. Bensahel, L.T. Canham, S. Ossicini (Eds.), Optical Properties of Low Dimensional Silicon Structures, Kluwer, Dordrecht, Amsterdam, 1993. [Pg.274]


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Silicone structure

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