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Greens function Subject

In the cellular multiple scattering model , finite clusters of atoms are subjected to condensed matter boundary conditions in such a manner that a continuous spectrum is allowed. They are therefore not molecular calculations. An X type of exchange was used to create a local potential and different potentials for up and down spin-states could be constructed. For uranium pnictides and chalcogenides compounds the clusters were of 8 atoms (4 metal, 4 non-metal). The local density of states was calculated directly from the imaginary part of the Green function. The major features of the results are ... [Pg.282]

The solution of Equation A-3 for the Green s function, subject to the boundary conditions in Equations A-6c and A-6d, is ... [Pg.48]

In mathematical terms, the implementation of the eigenstrain concept is carried out by representing the geometrical state of interest by some distribution of stress-free strains which can be mapped onto an equivalent set of body forces, the solution for which can be obtained using the relevant Green function. To illustrate the problem with a concrete example, we follow Eshelby in thinking of an elastic inclusion. The key point is that this inclusion is subject to some internal strain e, such as arises from a structural transformation, and for which there is no associated stress. [Pg.71]

We now argue that, for finite t, rejecting moves is the choice with the smaller time-step error when the importance-sampled Green function is employed. Sufficiently close to a node, the component of the velocity perpendicular to the node dominates all other terms in the Green function and it is illuminating to consider a free particle in one dimension subject to the boundary condition that have a node at x = 0. The exact Green function for this problem is... [Pg.103]

For H at T in Si, Katayama-Yoshida and Shindo (1983, 1985) used a Green s function method to carry out spin-density-functional calculations. They found a reduction of the spin density by a factor 0.41. However, their results are subject to some uncertainty because they obtained an erroneous result for the position of the defect state in the band gap, probably due to an insufficiently converged LCAO basis set. [Pg.624]

Figure 3. Distribution of C in plant tissues as a function of solubility. Barley, corn, cotton, peanut cell cultures, and soybeans were treated with V C] PCNB for 3 days. Lake water rich in blue green algae was treated for 9 h. Peanut plants were treated for 2 days and subjected to a 2-day post-treatment incubation. Figure 3. Distribution of C in plant tissues as a function of solubility. Barley, corn, cotton, peanut cell cultures, and soybeans were treated with V C] PCNB for 3 days. Lake water rich in blue green algae was treated for 9 h. Peanut plants were treated for 2 days and subjected to a 2-day post-treatment incubation.
Finally, for completeness, the Green s function corresponding to a pair of reactants initially formed with separation r0 and subjected to the partially reflecting boundary condition, is quoted (Pagistas and Kapral [37], Naqvi et al. [38]. [Pg.24]

Very much more effort on the subject of diffusion-limited reaction rates has been devoted to theoretical aspects, most of which has been with the aid of the diffusion equation. Indeed, so much has now been written that there are many articles which have not even been mentioned here. Yet it should be emphasised that much of what can be usefully said about the theoretical analysis of reaction rates with the diffusion equation has been said, sometimes several times, for which the author takes some share of responsibility Both the subjects of homogeneous reaction and pair recombination have been exhaustively analysed. Because the molecular pair approach is identical to the diffusion equation analysis, if the Noyes h(t) expression is approximated by a diffusive Green s function, no further effort on the molecular pair approach is really necessary. [Pg.252]

So far, the Lagrangian density for a homogenous problem (no sink or source term in the diffusion equation) has been considered, subject to the requirement that the approximate trial function, ip, can be forced to satisfy the boundary conditions. In this sub-section, these limitations are removed and the Lagrangian density for the Green s function developed. The Green s functions for the forward and backward time process satisfy the equations... [Pg.302]

Such purely mathematical problems as the existence and uniqueness of solutions of parabolic partial differential equations subject to free boundary conditions will not be discussed. These questions have been fully answered in recent years by the contributions of Evans (E2), Friedman (Fo, F6, F7), Kyner (K8, K9), Miranker (M8), Miranker and Keller (M9), Rubinstein (R7, R8, R9), Sestini (S5), and others, principally by application of fixed-point theorems and Green s function techniques. Readers concerned with these aspects should consult these authors for further references. [Pg.77]

Stacy, R.W., D.House, M.Friedman, M.Hazucha, J.Green, L.Raggio, and L.J.Roger. 1981. Effects of 0.75 ppm sulfur dioxide on pulmonary function parameters of normal human subjects. [Pg.308]


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