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Semiconductor atoms

So far, we have focused our attention on adsorption of donor particles on semiconductor oxides. As for the effect of adsorption of acceptor particles on electrophysical characteristics, in concurrence with conclusions made none of adsorption phenomenon involving such characteristic acceptor particles as molecular and atom oxygen on -semiconductor, atoms of nitrogen and simplest alkyl and amine radicals brought about a non-monotonous change in characteristics of adsorbents, despite the fact that experiments had been conducted at various conditions. [Pg.50]

The carbides with the NaCl structure may be considered to consist of alternating layers of metal atoms and layers of semiconductor atoms where the planes are octahedral ones of the cubic symmetry system. (Figure 10.1). In TiC, for example, the carbon atoms lie 3.06A apart which is about twice the covalent bond length of 1.54 A, so the carbon atoms are not covalently bonded, but they may transfer some charge to the metal layers, and they do increase the valence electron density. [Pg.132]

In a supercell geometry, which seems to have become the method of choice these days, the impurity is surrounded by a finite number of semiconductor atoms, and what whole structure is periodically repeated (e.g., Pickett et al., 1979 Van de Walle et al., 1989). This allows the use of various techniques that require translational periodicity of the system. Provided the impurities are sufficiently well separated, properties of a single isolated impurity can be derived. Supercells containing 16 or 32 atoms have typically been found to be sufficient for such purposes (Van de Walle et al., 1989). The band structure of the host crystal is well described. [Pg.603]

Fig. 5. (a) Schematic illustration of orbitals in the bond-center configuration. X and Y are the semiconductor atoms, (b) Corresponding energy levels obtained from simple molecular-bonding (or tight-binding) arguments for an elemental semiconductor... [Pg.616]

This simple treatment, formulated in a context of molecular bonding, was also what led Cox and Symons (1986) to propose the bond-center site as an explanation for anomalous muonium (Mu ). The location of the muon at the nodal plane of the nonbonding orbital explains the very small hyperfine coupling observed in pSR. Still, the muon is close to the electron, which occupies a nonbonding state on the neighboring semiconductor atoms. [Pg.617]

Semiconductors Atoms, molecules, and Campus drinking Superfund sites in... [Pg.40]

Fig. 6.17 Free energy surfaces for the InP-liquid interface calculated from the molecular orbital molecular dynamics (MD). The solid curve is for the case of fixed semiconductor atoms the dashed curve is calculated by including the dynamics of the semiconductor atoms. (After ref. [24])... Fig. 6.17 Free energy surfaces for the InP-liquid interface calculated from the molecular orbital molecular dynamics (MD). The solid curve is for the case of fixed semiconductor atoms the dashed curve is calculated by including the dynamics of the semiconductor atoms. (After ref. [24])...
The levels structure of the EM acceptor centres is determined by the characteristics of the VB of their host crystal near from its absolute extremum. As mentioned before, this extremum is located at k = 0 in most semiconductors. The contribution of the atomic p states of the constituent semiconductor atoms is predominant in the VB (for the compound crystals, it is related to the most electronegative atom). When spin-orbit (s-o) coupling is included, the pseudo-angular momentum J associated with the upper VB is L + S where L = 1 corresponds to the p electrons of the host crystal. For this reason and since they correspond to the pseudo-angular momenta J = 3/2 and 1/2, in the description of the acceptor states in diamond-type semiconductors, the T8 and r7- VBs are often labelled the p3/2 and j> /2 bands, respectively. [Pg.148]

Solid-state synthesis of this type draws the special attention in connection with an opportunity to prepare and stabilize small clusters of metal or semiconductor atoms in a polymeric matrix at ambient and even higher temperatures. Size-dependent quantum states in such clusters, which are the intermediate form between metal atoms and bulk metal, can give new electronic, optical, and magnetic effects [80]. The structure and properties of clus-... [Pg.70]

The transition of metal or semiconductor atoms into cations or complexes is the anodic subprocess. The electrons delivered by this process must be consumed by an outer electrical current or by a cathodic subprocess in order to keep the electrode potential high enough for the etching. As well as transport control in the anodic subprocess, the cathodic process can also be transport-controlled. The convection and the concentration of oxidizing agent inside solution are responsible together for the intensity of the cathodic process. The cathodic process does not occur... [Pg.881]

Some inorganic covalent compounds are crystalline solids built by covalent bonds. Some of these types of compounds are important functional materials, such as compound semiconductors. Atomic parameters such as covalent radius and electronegativity are useful atomic parameters for the investigation of these materials. [Pg.104]

In the third step, our ZT-TBMD method has been extended by incorporating the Nose-bath (Nose 1984) and the Multiple Histogram approximations (Fanourgakis et al. 1997), so as to be applicable to cluster studies at finite temperatures in an efficient way (Andriotis et al. 2006, 2007 Fthenakis et al. 2003). This generalization allows one to calculate the caloric curve for the cluster and use this to study the effect of temperature on the structural, electronic, and magnetic properties of transition metal clusters and binary systems containing transition metal and semiconductor atoms. The method has been used to study the variation of structural and magnetic properties with temperature as well as to obtain the caloric curves of the Ni-clusters (Andriotis et al. 2006,2007 Fthenakis et al. 2003). [Pg.946]

X-doped Au clusters (X=transition metal, semiconductor atoms, sulfur) show distinctive structural, electronic and magnetic properties. Wang et al. made a comprehensive comparison between DFT-based BH structure searches and experimental trapped ion electron diffraction and photo electron spectroscopic data on transition metal (Fe, Co, and Ni) doped Aui6 cluster. They found agreement between theoretical and... [Pg.270]


See other pages where Semiconductor atoms is mentioned: [Pg.42]    [Pg.601]    [Pg.610]    [Pg.611]    [Pg.620]    [Pg.586]    [Pg.595]    [Pg.596]    [Pg.605]    [Pg.287]    [Pg.88]    [Pg.205]    [Pg.269]    [Pg.269]    [Pg.149]    [Pg.1468]    [Pg.122]    [Pg.28]    [Pg.28]    [Pg.121]    [Pg.259]    [Pg.351]    [Pg.25]    [Pg.449]    [Pg.120]    [Pg.205]    [Pg.213]   
See also in sourсe #XX -- [ Pg.60 ]




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Atom Probe Studies of Semiconductor Materials

Atom probe semiconductors

Atomic Model of Semiconductor Quantum Dots

Atomic adsorption on compound semiconductors

Atomic adsorption, semiconductor

Atomic adsorption, semiconductor surfaces

Atomically clean semiconductor surfaces

Network atomic solids semiconductor

Semiconductor Nanocrystals as Artificial Atoms

Semiconductor atomic density

Semiconductor dots, confined atoms

Surface atom ionization of covalent semiconductor electrodes

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