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The Single Crystal

In addition to the periodicity of the crystal lattice, there are other factors affecting the diffraction quality of the crystal, i.e. the type of the ordered atoms have a significant influence on the diffraction power of the crystal. The heavier (more electrons) [Pg.309]


Most fiindamental surface science investigations employ single-crystal samples cut along a low-index plane. The single-crystal surface is prepared to be nearly atomically flat. The surface may also be modified in vacuum. For example, it may be exposed to a gas that adsorbs (sticks) to the surface, or a film can be grown onto a sample by evaporation of material. In addition to single-crystal surfaces, many researchers have investigated vicinal, i.e. stepped, surfaces as well as the surfaces of polycrystalline and disordered materials. [Pg.283]

The formation of such materials may be monitored by several techniques. One of the most useful methods is and C-nmr spectroscopy where stable complexes in solution may give rise to characteristic shifts of signals relative to the uncomplexed species (43). Solution nmr spectroscopy has also been used to detect the presence of soHd inclusion compound (after dissolution) and to determine composition (host guest ratio) of the material. Infrared spectroscopy (126) and combustion analysis are further methods to study inclusion formation. For general screening purposes of soHd inclusion stmctures, the x-ray powder diffraction method is suitable (123). However, if detailed stmctures are requited, the single crystal x-ray diffraction method (127) has to be used. [Pg.74]

The typical industrial catalyst has both microscopic and macroscopic regions with different compositions and stmctures the surfaces of industrial catalysts are much more complex than those of the single crystals of metal investigated in ultrahigh vacuum experiments. Because surfaces of industrial catalysts are very difficult to characterize precisely and catalytic properties are sensitive to small stmctural details, it is usually not possible to identify the specific combinations of atoms on a surface, called catalytic sites or active sites, that are responsible for catalysis. Experiments with catalyst poisons, substances that bond strongly with catalyst surfaces and deactivate them, have shown that the catalytic sites are usually a small fraction of the catalyst surface. Most models of catalytic sites rest on rather shaky foundations. [Pg.171]

The total cerium content in the single crystal samples on the basis of rare-earth elements is determined by photometry after Ce(III) oxidation by ammonium persulfate. The Ce(III) content is calculated from the difference. Comparison of the determination results of the total cerium content obtained by photometric and atomic emission methods for Li GdlBO ljiCe demonstrated the elaborated procedure precision and systematic error absence. [Pg.198]

In the following discussion, heavy emphasis is made of examples from studies of adsorbed layers on metal single-crystal samples. These illustrate the power of the HREELS technique and represent the main use of HREELS historically. Certainly HREELS has been used outside of the single-crystal world, and mention is made concerning its use on practical materials. This latter use of HREELS represents a true frontier. [Pg.448]

The optimal network increases total residence time by 48 per cent when compared with an equivalent MSMPR of the same volume and throughput. This increase would translate into a similar increase in mean crystal size and a 78 per cent increase in yield. Exactly the same residence time as for the single crystallizer have been reported from simple cascade configurations previously designed for stage-wise crystallization processes for slight improvements in... [Pg.285]

The single crystal of a polymer is a lamellar structure with a thin plateletlike form, and the chain runs perpendicular to the lamella. The crystal is thinner than the polymer chain length. The chain folds back and forth on the top and bottom surfaces. Since the fold costs extra energy, this folded chain crystal (FCC) should be metastable with respect to the thermodynamically more stable extended chain crystal (ECC) without folds. [Pg.905]

On the other hand, in the single crystals prepared from equivalent amounts of heterochiral 1 1 complexes, a pair of two heterochiral 1 1 complexes are incorporated in a unit cell to form a layered structure with alternate layer distances of 7.33 and 7.6 A. Two perchlorate ions stay in the narrower gap, and two additional acetone molecules as crystallization solvent occupy the wider gap. The perchlorate ions interact with two axial water ligands by hydrogen bonds (3.71 and 3.77 A) to construct a layered structure. The adjacent two molecules of heterochiral 1 1 com-... [Pg.265]

The silicon wafers used in conventional microelectronics arc fragile, relatively expensive, and their size is limited to that of the single-crystal ingot from which they are cut. In applications where large areas arc required, other materials seem... [Pg.251]

Several b-polarized sharp bands are assigned as ground slate totally symmetric vibrations at 699, 738, 1056, 1369, 1460 and 1504 cnT1 built on the fluorescence origin (see Fig. 6-18). These modes are in excellenl agreement with those obtained from the single crystal Raman spectra thal we measured exciting at 1064 and 632.8 nm [35]. [Pg.415]

In this article we have reviewed the results of a joint spectroscopic and morphological investigation of -sexilhienyl (T(J. The lowest singlet electronic level, which is assigned to I B , splits in the single crystal into four crystalline levels. The structure of the exciton band is investigated by the combined absorption and... [Pg.420]

For the three oclyloxy-subslitulcd five-ring oligomers, the normalized photoluminescence spectra of the single crystals are depicted in Figure 16-26. Due to the large absorption coefficient (more than 105 cm"1 at the maximum) we were not able to measure the absorption spectra of the relatively thick (20-30 pm) single crystals (see Table 16-5 in Section 16.3.3.3.1). [Pg.617]


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Abstraction from Single-Crystal Silicon—the Molecular Beam Method

Diffraction by single crystals the theoretical basis

Growth of Single Crystals from the Melt

Introduction to the Growth of Single Crystals

Orientation in the thermoplastic elastomers macroscopic single crystals

Single-crystal structure of a-Fe and the active sites

Structure of the Hydrogen Wave and Experiments on Single-Crystal Planes

The Single-Crystal Method of Studying Surface Reactions

The growth of single crystals

The structure of single crystal surfaces

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