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Correlations layer

The build-up process is mostly simulated by adding to a central unit successive correlation layers which saturate the bonds let free in the precedent layer. It comes nearest to the conditions under which a film is deposited. In this phase rules have to be introduced in order to achieve ideality or randomness . An alternative way of building a model starts from a completely disordered system of atoms which are then shifted in small steps so as to occupy the correct distances to the nearest and next-nearest neighbours (Henderson (1971). It comes nearest to the process of quenching a melt. [Pg.87]

Fig. 2.34. Energy of tetrahedrally bound atom clusters of different structures (s/e - ratio between staggered and eclipsed bonds) and sizes (N - number of correlation layers) (after Grigorovici and M iilJl (1969)). Fig. 2.34. Energy of tetrahedrally bound atom clusters of different structures (s/e - ratio between staggered and eclipsed bonds) and sizes (N - number of correlation layers) (after Grigorovici and M iilJl (1969)).
Polk s random network model confirmed many essential features of the Grigorovici-M aila continuous network model Uke the mixing of merged 5-and 6-fold rings in about the same ratio, the overlap of correlation layers on the r scale, the possibility to extend the model without limits, etc. Due to the peculiarities of the ball-and-spoke units he used, the increase in the... [Pg.92]

Fig. 2.35. The histogram of an ideal random continuous network model of a-Ge or a-Si (after Polk (1971)). Horizontally shaded area - first correlation layer diagonally shaded area - second correlation layer vertically shaded area - third- and higher order correlation layers. Full curve - RDF of a-Si (after Moss and Graczyk (1969)). Fig. 2.35. The histogram of an ideal random continuous network model of a-Ge or a-Si (after Polk (1971)). Horizontally shaded area - first correlation layer diagonally shaded area - second correlation layer vertically shaded area - third- and higher order correlation layers. Full curve - RDF of a-Si (after Moss and Graczyk (1969)).
Secondly, the linearized inverse problem is, as well as known, ill-posed because it involves the solution of a Fredholm integral equation of the first kind. The solution must be regularized to yield a stable and physically plausible solution. In this apphcation, the classical smoothness constraint on the solution [8], does not allow to recover the discontinuities of the original object function. In our case, we have considered notches at the smface of the half-space conductive media. So, notche shapes involve abrupt contours. This strong local correlation between pixels in each layer of the half conductive media suggests to represent the contrast function (the object function) by a piecewise continuous function. According to previous works that we have aheady presented [14], we 2584... [Pg.326]

Fig. 3 Refraction values of both (0°+ 90°) fiber directions with respect to impact energy per layer. The fiber/matrix debonding of CFRP laminates correlates significantly to the impact energy per volume (energy density). Fig. 3 Refraction values of both (0°+ 90°) fiber directions with respect to impact energy per layer. The fiber/matrix debonding of CFRP laminates correlates significantly to the impact energy per volume (energy density).
The most popular of the scanning probe tecimiques are STM and atomic force microscopy (AFM). STM and AFM provide images of the outemiost layer of a surface with atomic resolution. STM measures the spatial distribution of the surface electronic density by monitoring the tiumelling of electrons either from the sample to the tip or from the tip to the sample. This provides a map of the density of filled or empty electronic states, respectively. The variations in surface electron density are generally correlated with the atomic positions. [Pg.310]

Figure A2.4.11. Water pair correlation functions near the Pt(lOO) surface. In each panel, the frill curve is for water molecules in the first layer, and the broken curve is for water molecules in the second layer. From [30]. Figure A2.4.11. Water pair correlation functions near the Pt(lOO) surface. In each panel, the frill curve is for water molecules in the first layer, and the broken curve is for water molecules in the second layer. From [30].
This intensity can be used to calculate the correlation fiinction (Bl.9.101) and the interface distribution fiinction (B 1.9.102) and to yield the lamellar crystal and amorphous layer thicknesses along the fibre. [Pg.1408]

These pairs of encoded structures and their (R spectra are used to ti ain a counterpropagation network (see Section 9.5.5). The two-layer netwoi k pi ocesses the structural information in its upper part and the spectral information in its lower part. Thus the network learns the correlation between the structures and their (R spec tra. This prnciedine is shown in Figine 10.2-8. [Pg.531]

Another concept sometimes used as a basis for comparison and correlation of mass transfer data in columns is the Clulton-Colbum analogy (35). This semi-empirical relationship was developed for correlating mass- and heat-transfer data in pipes and is based on the turbulent boundary layer model... [Pg.23]


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