Definition local density approximation

Local density of states (continued) definition 119 s-wave-tip model, and 29 Sommerfeld metal 93 STM corrugation, and 142 total charge density, and 120 Local modification of sample wavefunctions 195 Local-density approximation 114 Logarithmic amplifier 257 Louse 269... 

Table II presents the first excitation energies obtained from spin- polarized calculations [24]. As ground-state exchange-correlation potentials were used the extra term in Eq.(20) does not appear. This is, certainly, one of the reasons for the difference between the calculated and the experimental excitation energies. There is a definite improvement comparing with the nonspin-polarized results [13]. Still, in most cases the calculated excitation energies are highly overestimated. The results provided by the different local density approximations are quite close to each other. The best one seems to be the Gunnarson-Lundqvist-Wilkins approximation. (In non-spin-polarized case the Perdew-Zunger parametrization gives results closest to the experimental data[30].)...

In order to solve these problems, it is very important and useful to clarify band structures of group-III nitrides and their QW structures and also to obtain their band structure parameters. In this Datareview, definitions of band structure parameters and available data on them for GaN and AIN are given. The data are mainly about theoretical results with first-principles band structure calculations within the local density functional approximation (LDA). They are compared with currently available experimental results. Note that the LDA calculation grossly underestimates a bandgap and that it gives almost zero bandgap for InN. Such a calculation is unlikely to yield reliable parameters for InN, especially effective masses. Therefore, the band structure parameters of InN are not given in this Datareview. 

HJ point out that in the detailed work on H2 by Kolos and Wolniewicz,114 the first excited state 3 2 was found to have a very weak minimum at a large separation. This binding presumably arises from a van der Waals force which is not included in the density functional theory when a local approximation to exchange and correlation is employed. Nevertheless, as HJ point out, their study of the corresponding state of the dimers Li2-Cs2 revealed a weak, but definite maximum in each case. Rough estimates of binding energy and equilibrium separation are shown in Table 16. It is, of course, possible that these results are a consequence of the local spin-density approximation, so that further work will... 

The kinetic theory leads to the definitions of the temperature, pressure, internal energy, heat flow density, diffusion flows, entropy flow, and entropy source in terms of definite integrals of the distribution function with respect to the molecular velocities. The classical phenomenological expressions for the entropy flow and entropy source (the product of flows and forces) follow from the approximate solution of the Boltzmann kinetic equation. This corresponds to the linear nonequilibrium thermodynamics approach of irreversible processes, and to Onsager s symmetry relations with the assumption of local equilibrium. 

The ProDos differs from the usual partial density of states (PDOS) calculated in the previous works in the definition (6). The summation in the Eq. (7) is over the unoccupied final states, thus N iE) will be proportional to the absorption cross section approximately (5). However, ProDos and PDOS are nearly the same, as far as the localized bound states are concerned. We have found that the ProDos of our clusters are very similar to PDOS of them. In this report, we concentrate our discussions on ProDOS of the central atom Ti to compare them with the XAS results of Ti40, (7). 

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