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Atomic image type

The two methiodides 23 and 25 give rise to (—), and (+ )-anhydro-lycorine methiodides (29) and (30) respectively, which differ on the basis of the absolute configuration of the quaternary nitrogen atom. The ORD and CD curves of (+ )-anhydrolycorine a-methiodide (30) in aqueous solution showed a high-intensity positive Cotton effect at 240 nm while the curves of (— )-anhydrolycorine /8-methiodide (29) are of the mirror image type. [Pg.93]

Where 0ae(r) is the interaction between two atoms of type a and B and r v means the minimum image distance consistent with periodic boundary conditions. In addition, there can be... [Pg.128]

The (100), (110), and (HI) surfaces of homoepitaxial diamond layers, grown on type Ila diamonds by HFCVD, were observed by an atmospheric AFM in Ref [145]. On the (100) surface, there was indication of the presence of 2 x 1 reconstructed dimers, though no atomic image was observed. Other surfaces were found to be quite rough. A STM study of (111) faces on polycrystalline... [Pg.85]

Fig. 2. (A) Atomic resolution STM image of a carbon tube, 35 A in diameter. In addition to the atomic honeycomb structure, a zigzag superpattern along the tube axis can be seen. (B) "Ball-and-stick" structural model of a Cg(,-based carbon tube. The upper part is closed by a Cgo hemisphere cap. (C) Structural model of a giant superpattern produced by two misoriented graphitic sheets. The carbon atoms in the first layer are shaded, and the second layer atoms are open. Between the two dashed lines, we highlight those first layer atoms with white that do not overlap with second layer atoms. Because of their higher local density of states at the Fermi level, these atoms (p-type atoms) appear particularly bright in STM images (16,21). [ results in a zigzag superpattern along the tube axis within the two white dashed lines as indicated. Fig. 2. (A) Atomic resolution STM image of a carbon tube, 35 A in diameter. In addition to the atomic honeycomb structure, a zigzag superpattern along the tube axis can be seen. (B) "Ball-and-stick" structural model of a Cg(,-based carbon tube. The upper part is closed by a Cgo hemisphere cap. (C) Structural model of a giant superpattern produced by two misoriented graphitic sheets. The carbon atoms in the first layer are shaded, and the second layer atoms are open. Between the two dashed lines, we highlight those first layer atoms with white that do not overlap with second layer atoms. Because of their higher local density of states at the Fermi level, these atoms (p-type atoms) appear particularly bright in STM images (16,21). [ results in a zigzag superpattern along the tube axis within the two white dashed lines as indicated.
Complete MCP s can be stacked to provide even higher gains. For response in the vacuum ultra-violet spectral region (50-200 nm) a SSANACON, self-scanned anode array with microchannel plate electron multiplier, has been used (36). This involves photoelectron multiplication through two MOP S, collection of the electrons directly on aluminum anodes and readout with standard diode array circuitry. In cases where analyte concentrations are well above conventional detection limits, multi-element analysis with multi-channel detectors by atomic emission has been demonstrated to be quite feasible (37). Spectral source profiling has also been done with photodiode arrays (27.29.31). In molecular spectrometry, imaging type detectors have been used in spectrophotometry, spectrofluometry and chemiluminescence (23.24.26.33). These detectors are often employed to monitor the output from an HPLC or GC (13.38.39.40). [Pg.61]

Fig. 19 Evolutionary optimisation at the atomic level. A combination of rule-based and genetic algorithm strategies is used to coerce an STM tip to produce one of two distinct image types, with no human operator involvement, (a) and (b) are the experimental images (c) and (d) the target structures (e) and (f) show profiles along the lines shown in (a) and (b). From Ref. 82. Fig. 19 Evolutionary optimisation at the atomic level. A combination of rule-based and genetic algorithm strategies is used to coerce an STM tip to produce one of two distinct image types, with no human operator involvement, (a) and (b) are the experimental images (c) and (d) the target structures (e) and (f) show profiles along the lines shown in (a) and (b). From Ref. 82.
AFM measures the spatial distribution of the forces between an ultrafme tip and the sample. This distribution of these forces is also highly correlated with the atomic structure. STM is able to image many semiconductor and metal surfaces with atomic resolution. AFM is necessary for insulating materials, however, as electron conduction is required for STM in order to achieve tiumelling. Note that there are many modes of operation for these instruments, and many variations in use. In addition, there are other types of scaiming probe microscopies under development. [Pg.310]

Chiral separations are concerned with separating molecules that can exist as nonsupetimposable mirror images. Examples of these types of molecules, called enantiomers or optical isomers are illustrated in Figure 1. Although chirahty is often associated with compounds containing a tetrahedral carbon with four different substituents, other atoms, such as phosphoms or sulfur, may also be chiral. In addition, molecules containing a center of asymmetry, such as hexahehcene, tetrasubstituted adamantanes, and substituted aHenes or molecules with hindered rotation, such as some 2,2 disubstituted binaphthyls, may also be chiral. Compounds exhibiting a center of asymmetry are called atropisomers. An extensive review of stereochemistry may be found under Pharmaceuticals, Chiral. [Pg.59]

New types of scanning probe microscopies are continually being developed. These tools will continue to be important for imaging of surfaces at atomic-scale resolution. [Pg.274]

A special mention is in order of high-resolution electron microscopy (HREM), a variant that permits columns of atoms normal to the specimen surface to be imaged the resolution is better than an atomic diameter, but the nature of the image is not safely interpretable without the use of computer simulation of images to check whether the assumed interpretation matches what is actually seen. Solid-state chemists studying complex, non-stoichiometric oxides found this image simulation approach essential for their work. The technique has proved immensely powerful, especially with respect to the many types of defect that are found in microstructures. [Pg.221]

Figure 9.1 Tetrahedral carbon atoms and their mirror images. Molecules of the type CH3X and CH2XY are identical to their mirror images, but a molecule of the type CHXYZ is not. A CHXYZ CH3X X l X hK vh H ... Figure 9.1 Tetrahedral carbon atoms and their mirror images. Molecules of the type CH3X and CH2XY are identical to their mirror images, but a molecule of the type CHXYZ is not. A CHXYZ CH3X X l X hK vh H ...
Several types of atoms in addition to hydrogen can be detected by MRI, and the applications of images based on 31P atoms are being explored. The technique holds great promise for studies of metabolism. [Pg.469]


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Atom types

Atom typing

Atomic imaging

Atoms images

Types atomic

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