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Crystals and Films

Lead sulfide films have been prepared by various deposition processes like vacuum evaporation and chemical bath deposition. Electrochemical preparation techniques have been used in a few instances. Pourbaix diagrams for all three aqueous lead-chalcogen Pb-S, Pb-Se, and Pb-Te systems, along with experimental results and cited discussion on the chemical etching and electrolytic polishing of lead chalcogenide crystals and films, have been presented by Robozerov et al. [201]. [Pg.124]

Beginning with a discussion of the necessary basic physics and chemistry, the book proceeds to a description of the main topics of current research in this field. The Langmuir-Blodgett technique, self-assembly, and methods of film deposition exploiting the ordered structure of mesophases are discussed. Separate chapters are devoted to the properties and computer modelling of both liquid crystals and films at the air/water interface. Order in biomemebranes is also discussed. [Pg.200]

Parameter defining the acoustic matching of a crystal and film material... [Pg.98]

On Fig. 13 the desorption energy at a coverage close to zero is plotted as a function of the particle size. We see that it increases from around 30 kcal/mol at a size of 5 nm (or larger) up to 38 kcal/mol for a size of about 2 nm. The increase of the desorption energy, at nearly zero coverage, as the Pd particle size decreases has been observed for several supports (MgO, mica, A1203 single crystal and film) as seen in Table 1. [Pg.266]

Rack JJ, Winkler JR, Gray HB. Phototriggered Ru(II)-dimethylsulfoxide linkage isomerization in crystals and films. J Am Chem Soc 2001 123 2432-3. [Pg.71]

Since crystal and film are fixed, only a small part of reciprocal space can be observed at a time, but a reciprocal point of the diffracting volume scatters during the whole exposure time. By contrast, scanning techniques such as Weissenberg or precession cameras see a larger part of reciprocal space, but each reciprocal point stays only a short time on the Ewald sphere. [Pg.188]

Diamonds electrical measurement EPR spectrometry diamond crystals and films... [Pg.299]

Formation of twin structures on the faces of diamond crystals and films have also been studied by Koidl s group in the early stage of diamond film research [84], So, we begin with reviewing their works, which is then followed by studies of other groups. To make heteroepitaxial diamond films, it is necessary to avoid the formation of twins, and thus the studies on the formation mechanism and morphology of twins are of great importance. [Pg.53]

There are two variations of the Laue method, depending on the relative positions of source, crystal, and film (Fig. 3-5). In each, the film is flat and placed perpendicular to the incident beam. The film in the transmission Laue method (the original Laue method) is placed behind the crystal so as to record the beams diffracted in the forward direction. This method is so called because the diffracted beams are partially transmitted through the crystal. In the back-reflection Laue method the film is placed between the crystal and the x-ray source, the incident beam passing through a hole in the film, and the beams diffracted in a backward direction are recorded. [Pg.92]

This observation paves the way to the work by Tsiper and Soos that proposed a mean-field approximation for the calculation of the linear polarizability of molecular crystals and films [25, 62, 63, 64]. The approach is based again on the neglect of intermolecular overlap. A quantum chemical model is adopted for each molecular... [Pg.259]

In the following, various CVD techniques for the growth of diamond crystals and films on deposition substrates are discussed in detail. [Pg.18]

In the combustion synthesis of diamond crystals and films on Mo substrates,by reducing the O2/C2H2 ratio in the gas mixture to 0.75... [Pg.118]

Van Hutten, P.R, V.V. Krasnikov, H.J. Brouwer, and G. Hadziioannou. 1999. Excimer luminescence from single crystals and films of a cyano-substituted phenylene-vinylene model compound. Chem Phys 241 139 -154. [Pg.1273]

In some instances materials with potentially useful properties have not been exploited until prepared as pure crystals and films. Examples of this include doped poly thi-azyl, (SN), and polyacetylene, (CH) c, which have metallic properties, including electrical conductivity. The use of polymer precursors for ceramics (e.g., silicon carbide) is another interesting solid-state preparation technique. [Pg.274]

The ability to image organic crystals and films with molecular-scale contrast enables determination of the lattice parameters of the imaged plane, while step heights can provide the lattice constant normal to the plane. Consequently, AFM can be useful for identification or confirmation of crystal structure. AFM and crystallographic dimensions will typically differ by <5%. These differences may be attributed partially to measurement error inherent in the AFM, although surface reconstruction with concomitant reduction in surface energy is also likely. Much of this data is acquired in Kquids, so reconstruction can also result from surface interaction with solvent molecules. [Pg.5853]

Second-harmonic generation for nonlinear optics, ferroelectricity, and piezoelectricity are all properties that are dependent on the pre.sence, magnitude, and orientation of bulk polarity in crystals and films. Therefore, the issue of how to design a polar solid from basic principles remains a challenge that has immense potential relevance to materials science. Obviously, a polar solid is guaranteed if a pure enantiomer is used as a component of a compound. However, the presence of polarity does not in any way imply that optimal packing will occur and, further-... [Pg.889]


See other pages where Crystals and Films is mentioned: [Pg.379]    [Pg.32]    [Pg.83]    [Pg.1]    [Pg.186]    [Pg.243]    [Pg.76]    [Pg.511]    [Pg.303]    [Pg.30]    [Pg.353]    [Pg.303]    [Pg.11]    [Pg.48]    [Pg.185]    [Pg.268]    [Pg.218]    [Pg.177]    [Pg.260]    [Pg.687]    [Pg.58]    [Pg.58]    [Pg.83]    [Pg.161]    [Pg.176]    [Pg.226]    [Pg.103]    [Pg.129]    [Pg.683]    [Pg.488]    [Pg.172]   


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Crystal Orientations and Film Surface Morphology

Microwave properties of dielectric single crystals, ceramics and thin films

Single crystal and epitaxial film electrodes

Thin Films in Complete Wetting and the Specific Case of Nematic Liquid Crystals

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