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Illustration 2 Reduced Dimensional Systems

How does the reduced dimensionality affect the dispersion relations Whangbo, Canadell and co-workers have qualitatively evaluated the band dispersion in such systems in the same way as was done for the three-dimensional perovskite strucmre in the last section - by counting the number of oxygen p orbital contributions present in the COs at certain points in the BZ. [Pg.231]

If the lowest energy point lies at F, predict the iowest-iying 2g- biock band for the n = 3 member of the Ruddiesden-Popper phase, which exhibits out-of-center octahedrai distortion in the outer iayers. Discuss the impiications on the eiectronic properties of oxides with iow d eiectron counts. [Pg.232]

The n = 3 member of the Ruddiesden-Popper phases have triple-layer vertexsharing octahedrai siabs separated by rock-sait-iike iayers. It is a iow-dimensionai transport system with nine 2g bands. These can be denoted xz, xz , xz , and so on, where denotes the d band of the centrai iayer of an M-O-M-O-M iinkage. [Pg.232]

Drawing the orbitais in the M-O-M-O-M iinkage aiiows one to count the antibonding contributions in each of these bands. Compared to that of the singie-iayer octahedrai siab, each xy band in the tripie-iayer siab wiii have three times as many O p orbitai contributions. Thexz and yz bands will have [Pg.232]

The implications are that conduction electrons confined to the inner-layer slab, in oxides with low d electron counts, may be more spatially screened from electron localizing effects such as chemical or structural disorder in the rock-salt-like slabs, as compared with conduction electrons in single-layer slabs. [Pg.233]


For larger hydrogen-bonded systems, rigorous calculations are far more difficult to carry out, both from the point of view of obtaining full-dimensional potentials and the subsequent quantum vibrational calculations. Reduced dimensionality approaches are therefore often necessary and several chapters in this volume illustrate this approach. With increasing computational power, coupled with some new approaches, it is possible to treat modest sized H-bonded systems in full dimensionality. We have already briefly reviewed the approach we have developed for potentials for the vibrations we have primarily used the code Multimode (MM). The methods used in MM have been reviewed recently [24 and references therein, 25], and so we only give a very brief overview of the method here. [Pg.59]

In this section we illustrate the application of the spherical-harmonics method by considering two problems of some practical interest. Both problems deal with steady-state one-dimensional systems, and the calculation is carried out on the basis of the one-velocity model developed in Sec. 7.2f. In the present applications the general time-dependent relations given in (7.84) reduce to the following set of differential equations ... [Pg.387]

ABSTRACT. In this paper, the theoretical basis and the program architecture of some reduced dimensionality quantum reactive scattering computational procedures are illustrated. The aim is to evidence to what extent it is possible to take advantage of parallel and vector performances of modem supercomputers for carrying out extensive calculations of the reactive properties of atom diatom systems. Some efforts have been paid to indicate alternative ways of formulating both the theoretical approaches and the computational codes. Speed-up factors of the suggested solutions have been calculated for some test cases. Results of extensive calculations performed for two prototype reactive systems are presented. [Pg.271]

Reduced dimensionality paired with interfacial interactions were discussed as the major source for constraints in mesoscale systems. Material constraints leading to the observation of exotic properties were documented and illustrated from various fields. Although on first sight, the findings fi om the different disciplines appeared to be unrelated, they can be interpreted on a similar basis with the proposed classification of interfacial sciences. [Pg.21]

In an axisymmetric flow regime all of the field variables remain constant in the circumferential direction around an axis of symmetry. Therefore the governing flow equations in axisymmetric systems can be analytically integrated with respect to this direction to reduce the model to a two-dimensional form. In order to illustrate this procedure we consider the three-dimensional continuity equation for an incompressible fluid written in a cylindrical (r, 9, 2) coordinate system as... [Pg.113]

This problem illustrates the solution approach to a one-dimensional, nonsteady-state, diffusional problem, as demonstrated in the simulation examples, DRY and ENZDYN. The system is represented in Fig. 4.2. Water diffuses through a porous solid, to the surface, where it evaporates into the atmosphere. It is required to determine the water concentration profile in the solid, under drying conditions. The quantity of water is limited and, therefore, the solid will eventually dry out and the drying rate will reduce to zero. [Pg.224]

This section concentrates on laminar premixed flames, which serve to illustrate many attributes of steady-state one-dimensional reacting systems. The governing equations themselves can be written directly from the more general systems derived in Chapter 3. Referring to the cylindrical-coordinate summary in Section 3.12.2, and retaining only the axial components, the one-dimensional flame equations reduce immediately to... [Pg.669]

Dimensional analysis, often referred to as the II-theorem is based on the fact that every system that is governed by m physical quantities can be reduced to a set of m - n mutually independent dimensionless groups, where n is the number of basic dimensions that are present in the physical quantities. The II-theorem was introduced by Buckingham [1] in 1914 and is therefore known as the Buckingham II-theorem. The II-theorem is a procedure to determine dimensionless numbers from a list of variables or physical quantities that are related to a specific problem. This is best illustrated by an example problem. [Pg.172]

The two-dimensional integral in Eq. (11.11) may be reduced to two one-dimensional integrals by a change of variables. This is illustrated in Fig. G.0.1, which shows a Cartesian coordinate system with unit axes (i,j) and associated coordinates t and T2-... [Pg.360]

A novel gradient-based optimisation framework for large-scale steady-state input/output simulators is presented. The method uses only low-dimensional Jacobian and reduced Hessian matrices calculated through on-line model-reduction techniques. The typically low-dimensional dominant system subspaces are adaptively computed using efficient subspace iterations. The corresponding low-dimensional Jacobians are constructed through a few numerical perturbations. Reduced Hessian matrices are computed numerically from a 2-step projection, firstly onto the dominant system subspace and secondly onto the subspace of the (few) degrees of freedom. The tubular reactor which is known to exhibit a rich parametric behaviour is used as an illustrative example. [Pg.545]


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Dimensional Systems

Dimensionality, reducing

Reduced dimensionality

Reduced systems

System dimensionality

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