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Tight-binding DFT

To conclude this section, and although we do not cover the TD-DFT and Tight-Binding DFT methods in this chapter we mention that extensions of the cDFT ideas of Dederich et al. have been developed for these methods. More generally, there is little doubt that further development of cDFT in the coming years will allow its application to numerous biologically relevant systems. [Pg.48]

As a consequence of the size limitations of the ab initio schemes, a large number of more-approximate methods can be found in the literature. Here, we mention only the density functional-based tight binding (DFTB) method, which is a two-center approach to DFT. The method has been successfully applied to the study of proton transport in perov-skites and imidazole (see Section 3.1.1.3). The fundamental constraints of DFT are (i) treatment of excited states and (ii) the ambiguous choice of the exchange correlation function. In many cases, the latter contains several parameters fitted to observable properties, which makes such calculations, in fact, semiempirical. [Pg.403]

In this paper we present preliminary results of an ab-initio study of quantum diffusion in the crystalline a-AlMnSi phase. The number of atoms in the unit cell (138) is sufficiently small to permit computation with the ab-initio Linearized Muffin Tin Orbitals (LMTO) method and provides us a good starting model. Within the Density Functional Theory (DFT) [15,16], this approach has still limitations due to the Local Density Approximation (LDA) for the exchange-correlation potential treatment of electron correlations and due to the approximation in the solution of the Schrodinger equation as explained in next section. However, we believe that this starting point is much better than simplified parametrized tight-binding like s-band models. [Pg.536]

The theoretical formalism for dealing with such a molecular device is the NEGF-DFT which has two different kinds of implementations. The implementation in [27,32,33] adopts a cluster approach in which the device scattering region (called extended molecule ) is calculated within DFT while the device leads are treated within tight-binding models. The main... [Pg.123]

Preliminary models of the surface topography, for example, can be determined by atomic-probe methods, ion-scattering, electron diffraction, or Auger spectroscopy. The chemical bonds of adsorbates can be estimated from infrared spectroscopy. The surface electronic structure is accessible by photoelectron emission techniques. In case the surface structure is known, its electronic structure has to be computed with sophisticated methods, where existing codes more and more rely on first principles density functional theory (DFT) [16-18], or, in case of tight-binding models [19], they obtain their parameters from a fit to DFT data [20]. The fit is not without ambiguities, since it is unknown whether the density of states used for the fit is really unique. [Pg.157]

The NRL tight-binding method has been used to address the adsorption of 02 on Pt(l 1 1) [99]. The Pt-Pt interactions were taken from a large data base of TB parameter for the elements which are posted on the world wide web [100]. These parameters were obtained from a fit to DFT bulk calculations. Still, it has been demonstrated that the pure Pt surface is also well-described by this parametrization [42], For the Pt-O and the 0-0 TB parameters a new fit had to be performed. They were adjusted in order to reproduce the GGA-DFT results of the 02/Pt(l 1 1) potential energy surface [91, 92], The root mean square error of the fit is below 0.1 eV [41] which is in the range of the error of the GGA-DFT calculations. The spin state of the oxygen molecule was not explicitly considered in the... [Pg.15]

The LCAO tight-binding (Hartree-Fock) method and its successor, the density-functional theory (DFT), were used originally to solve electronic structure problems. More recently, both have been applied to the calculation of total energy, which includes contributions due to core-core, core-electron, and electron-electron interactions. By varying the coordinates of the core, the dependence of the total energy on the core coordinates can be examined. This is referred... [Pg.70]

AMI Semiempirical Austin method 1 CSA Conformational space annealing DFT Density functional theory DFTB Density-functional-based tight binding EA Evolutionary algorithm... [Pg.33]

Figure 5. Molecular modeling methods at various scales. MO-miolecular orbital DFT-density functional theory TB-tight binding QM/MM-4iybrid quantum mechanics/molecular mechanics MD nolecnlar dynamics. Figure 5. Molecular modeling methods at various scales. MO-miolecular orbital DFT-density functional theory TB-tight binding QM/MM-4iybrid quantum mechanics/molecular mechanics MD nolecnlar dynamics.

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See also in sourсe #XX -- [ Pg.100 ]

See also in sourсe #XX -- [ Pg.2 ]

See also in sourсe #XX -- [ Pg.288 ]




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Tight-binding

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