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Next neighbors

Multilayers of Diphosphates. One way to find surface reactions that may lead to the formation of SAMs is to look for reactions that result in an insoluble salt. This is the case for phosphate monolayers, based on their highly insoluble salts with tetravalent transition metal ions. In these salts, the phosphates form layer stmctures, one OH group sticking to either side. Thus, replacing the OH with an alkyl chain to form the alkyl phosphonic acid was expected to result in a bilayer stmcture with alkyl chains extending from both sides of the metal phosphate sheet (335). When zirconium (TV) is used the distance between next neighbor alkyl chains is - 0.53 nm, which forces either chain disorder or chain tilt so that VDW attractive interactions can be reestablished. [Pg.543]

A, the radius of the No molecule is 0.545 A. In the PIMC simulations interactions up to the fourth neighbor shell were taken into account, the next neighbor shells (5-20) have been treated in a static lattice approximation, the rest in a continuum static approximation. [Pg.83]

Extended X-ray absorption fine structure (EXAFS) measurements based on the photoeffect caused by collision of an inner shell electron with an X-ray photon of sufficient energy may also be used. The spectrum, starting from the absorption edge, exhibits a sinusoidal fine structure caused by interferences between the outgoing and the backscattered waves of the photoelectron which is the product of the collision. Since the intensity of the backscattering decreases rapidly over the distances to the next neighbor atoms, information about the chemical surroundings of the excited atom can be deduced. [Pg.550]

The comparison reveals that in addition to the activity of individual atoms, the next-neighbor interaction and collective atomic motion must play an important role in creating friction. This mechanism can be investigated more efficiently via the Frenkel-Kontorova model. [Pg.176]

The reactivity of carbohydrates is dominated by the reactivity of the aldehyde group and the hydroxyl on its next-neighbor (/ ) carbon. As illustrated by the middle row of Fig. 2.3, the aldehyde can be isomerized to the corresponding enol or be converted into its hydrate (or hemiketal) form upon reaction with water (or with an hydroxyl-group). These two reactions are responsible for the easy cycliza-tion of sugars in five- and six-membered rings (furanose and pyranose) and their isomerization between various enantiomeric forms and between aldehyde- and ketone-type sugars (aldose and ketose). [Pg.29]

For k 1 (1 -NN), a new object would always get the same class membership as its next neighbor. Thus, for small values of k, it is easily possible that classes do no longer form connected regions in the data space, but they can consist of isolated clouds. The classification of new objects can thus be poor if k is chosen too small or too large. In the former case, we are concerned with overfitting, and in the latter case with underfitting. [Pg.229]

Note The term a-cleavage for this widespread radical-site initiated process with charge retention can be misleading, because the bond cleaved is not directly attached to the radical site, but to the next neighboring atom. [Pg.230]

The preceding considerations are essentially based on the model of random-matrix ensembles proposed by Dyson and others in the 1960s. Recent works, in particular by Casati and co-workers [89], have focused on band random matrices. Such matrices naturally arise in quantum systems with subspaces coupled only to next-neighboring subspaces such as for electronic states in a chain of atoms or in the kicked rotator. In such systems, localized states are observed that present a level statistics interme-... [Pg.518]

In contrast to that model, we generated statistical homogeneous defect structures with a broken coordination number of next neighbors. The exclusion volume of the segments should be accounted for. To our knowledge, there is no mathematical method that allows one to describe the radial distance distribution of such structures analytically. It must be calculated on a computer by generating the structure steadily. [Pg.66]

Any homogeneously distorted two-dimensional coordination scheme should be based upon the distance correlation statistics between next neighbors at least. In the case of a two-dimensional lattice construction, this distance correlation principle has been used by Hosemann and coworkers [13] to generate micro-paracrystals of finite size with the help of a computer. The construction procedure (known as spiral-paracrystal ) terminates if a coordination point cannot be assigned to a lattice point. [Pg.66]

First of all, a distance correlation function gNN(r) of next neighbors must be given. This function has to meet the following conditions ... [Pg.67]

Fig. 4. Distance distribution of next neighbors, approximated by a shifted Gaussian distribution (see text), r, = 3 A, = 5.1 A, a = 0.8 A... Fig. 4. Distance distribution of next neighbors, approximated by a shifted Gaussian distribution (see text), r, = 3 A, <r> = 5.1 A, a = 0.8 A...
Fig. 19. Variation of the cylinder length nZjl (number of CH2 units). The number of next neighbor... Fig. 19. Variation of the cylinder length nZjl (number of CH2 units). The number of next neighbor...
In the case of the PE melt, the largest part of the configuration entropy is included in the variety of chain conformations. In our model of the PE melt, these chain conformations cause the diameter of the correlation cylinders in which the chain segments are embedded to fluctuate. This leads necessarily to distance fluctuations of next neighbor segments because of steric hindrance of the local segment exclusion volume. Therefore, the inter- and intramolecular distance correlations cannot be discussed independently. [Pg.82]


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See also in sourсe #XX -- [ Pg.28 ]




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