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Silicon crystallization

Figure Al.3.22. Spatial distributions or charge densities for carbon and silicon crystals in the diamond structure. The density is only for the valence electrons the core electrons are omitted. This charge density is from an ab initio pseudopotential calculation [27]. Figure Al.3.22. Spatial distributions or charge densities for carbon and silicon crystals in the diamond structure. The density is only for the valence electrons the core electrons are omitted. This charge density is from an ab initio pseudopotential calculation [27].
The most connnonly used detector in EPR is a semiconducting silicon crystal in contact with a tungsten wire, which acts as an MW rectifier. At microwatt powers, crystal detectors are typically non-linear and render a... [Pg.1561]

This is demonstrated by the XPS spectra in figure B 1.25.5(a) which show the Si 2p spectra of a silicon crystal with a thin (native) oxide layer, measured under take-off angles of 0° and 60° [12]. When the take-off angle is... [Pg.1857]

Figure Bl.25.5. (a) XPS spectra at take-off angles of 0° and 60° as measured from the surface nonnal from a silicon crystal with a thin layer of Si02 on top. The relative intensity of the oxide signal increases significantly at higher take-off angles, illustrating that the surface sensitivity of XPS increases, (b) Plot of... Figure Bl.25.5. (a) XPS spectra at take-off angles of 0° and 60° as measured from the surface nonnal from a silicon crystal with a thin layer of Si02 on top. The relative intensity of the oxide signal increases significantly at higher take-off angles, illustrating that the surface sensitivity of XPS increases, (b) Plot of...
Under most circumstances the equiUbtium shape of silicon crystals is octahedral, ie, the slowest-growing faces are (111). However, external conditions can radically alter that shape. For example, when growth is from the vapor, concentration gradients in the gas stream may affect the shape, and when growth is from the melt, the shape is primarily determined by thermal gradients in the melt. [Pg.525]

Oxygen also dissolves in the silicon crystal lattice, forming SiO which may radically affect the electrical properties of the silicon. Oxygen is usually unintentionally introduced during the crystal-growing operation in concentrations up to the solubility limit (ca 2.5 x 10 atoms/cm ). When... [Pg.525]

The heart of the energy-dispersive spectrometer is a diode made from a silicon crystal with lithium atoms diffiised, or drifted, from one end into the matrix. The lithium atoms are used to compensate the relatively low concentration of grown-in impurity atoms by neutralizing them. In the diffusion process, the central core of the silicon will become intrinsic, but the end away from the lithium will remain p-type and the lithium end will be n-type. The result is a p-i-n diode. (Both lithium-... [Pg.122]

S. lida, Y. Aoki, K. Okitsu, Y. Sugita, H. Kawata, T. Abe. Microdefects in an as-grown Czochralski silicon crystal studied by synchrotron radiation section topography with aid of computer simulation. Jpn J Appl Phys Ptl 57 241, 1998. [Pg.926]

T. Sinno, R. A. Brown, W. Van Ammon, E. Dornberger. Point defect dynamics and the oxidation-induced stacking-fault ring in Czochralski-grown silicon crystals. J Electrochem Soc 145 302, 1998. [Pg.927]

J. Jaervinen, R. Nieminen, T. Tiihonen. Time-dependent simulation of Czochralski silicon crystal growth. J Cryst Growth 750 468, 1997. [Pg.928]

A. Muehlbauer, A. Muiznieks, J. Virbulis. Analysis of the dopant segregation effects at the floating zone growth of large silicon crystals. J Cryst Growth 750 372, 1997. [Pg.928]

In its ground state, the free atom Si has the electronic configuration [Ne]3s 3p. Ionization energies and other properties are compared with those of the other members of Group 14 on p. 372. Silicon crystallizes in the diamond... [Pg.330]

Even though silicon is metallic in appearance, it is not generally classified as a metal. The electrical conductivity of silicon is so much less than that of ordinary metals it is called a semiconductor. Silicon is an example of a network solid (see Figure 20-1)—it has the same atomic arrangement that occurs in diamond. Each silicon atom is surrounded by, and covalently bonded to, four other silicon atoms. Thus, the silicon crystal can be regarded as one giant molecule. [Pg.365]

It appears that a way to efficient electrochemical growth of CdTe and other chalcogenides on silicon crystals is the utilization of light-assisted processes. Works in this direction will be discussed in a subsequent section regarding underpotential deposition studies. [Pg.160]

At present, defect-free silicon crystals have been achieved at only at diameters of 200 mm. Comparisons of crystal quality were made among three techniques a typical conventional Czrochralski crystal growth technique, a slow-cooled controlled reaction and the perfect silicon process. The quality levels achieved in D-defect levels of the material is... [Pg.336]

A few ATR probes are commercially available. In the near-IR ATR probes are mostly used as easy-to-use sticking probes for liquids and solids. As the aim is primarily to identify a material, not to measure low concentrations, probes with typically one or two reflections (Figure 5-d) are used. In the mid-IR, similar layouts can be found, using e.g. zinc selenide, germanium or silicon crystals as sensing elements. More sensitive and generally better suited for industrial process control DiComp -type probes (Figure 5-e). The actual ATR element is in this case a thin diamond disc supported by a suitably shaped ZnSe crystal. ATR probes of that type are available off the shelf with between one and nine reflections. If more... [Pg.133]

In ultra pure crystalline silicon, there are no extra electrons in the lattice that can conduct an electric current. If however, the silicon becomes contaminated with arsenic atoms, then there will be one additional electron added to the silicon crystal lattice for each arsenic atom that is introduced. Upon heating, some of those "extra electrons will be promoted into the conduction band of the solid. The electrons that end up in the conduction band are able to move freely through the structure. In other words, the arsenic atoms increase the conductivity of the solid by providing additional electrons that can carry a current when they are promoted into the conduction band by thermal excitation. Thus, by virtue of having extra electrons in the lattice, silicon contaminated with arsenic will exhibit greater electrical conductance than pure silicon at elevated temperatures. [Pg.255]

Figure 1.6 (a) Donor impurity (PS ) in a silicon crystal. (b) Donor energy levels below the... [Pg.9]

Note that /lo(Es) is the inelastic mean free path of electrons formed in the substrate travelling through the overlayer. In the case that the overlayer is a film of Si02 on a silicon crystal, as in Fig. 3.13, Expression (3-9) reduces to... [Pg.71]


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See also in sourсe #XX -- [ Pg.90 , Pg.95 , Pg.99 , Pg.101 , Pg.102 ]




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Abstraction from Single-Crystal Silicon—the Molecular Beam Method

Application of MEM to single-crystal data on silicon

Bromine-silicon crystals

Crystal silicon carbides

Crystal silicon lattice structure

Crystal silicon nitrides

Crystal structure porous silicon

Crystallization amorphous silicon

Crystallization supercooled silicon

Free Single Crystal Silicon

Industrial silicon crystal

Photoaligned Liquid-Crystal-on-Silicon Microdisplays

Semiconductors silicon crystal structure

Silicon Nitride Single Crystals Mechanical Properties

Silicon Nitride Single Crystals Structure

Silicon carbide crystal growth

Silicon carbide single crystal

Silicon carbide, crystal structure

Silicon crystal

Silicon crystal growth

Silicon crystal native defect

Silicon crystal self-interstitials

Silicon crystal structure

Silicon crystal structure (diamond-like

Silicon crystal structure, mechanical and

Silicon crystal structures, lattice parameters

Silicon crystal surfaces

Silicon crystal vacancies

Silicon crystal, electron distribution

Silicon crystals, oxygen free

Silicon fibrous crystals

Silicon flat single-crystal

Silicon ionic crystal radius

Silicon melt crystal growth

Silicon monochromator crystal

Silicon seed crystals

Silicon single crystal

Silicon single crystal grains

Silicon single crystal, reflection

Silicon single-crystal ingots

Silicon single-crystal probe

Silicon skeleton crystals

Silicon ultrapure single-crystal

Silicon, crystal structure melting point

Silicon-based photonic crystals

Single-crystal electrolytes silicon

Single-crystal silicon nanowires

Single-crystal silicon wafers

The Carbon-Silicon Crystal Unit Cell

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