839 research outputs found

    Nearsightedness of Electronic Matter

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    In an earlier paper, W. Kohn had qualitatively introduced the concept of "nearsightedness" of electrons in many-atom systems. It can be viewed as underlying such important ideas as Pauling's "chemical bond," "transferability" and Yang's computational principle of "divide and conquer." It describes the fact that, for fixed chemical potential, local electronic properties, like the density n(r)n(r), depend significantly on the effective external potential only at nearby points. Changes of that potential, {\it no matter how large}, beyond a distance R\textsf{R} have {\it limited} effects on local electronic properties, which rapidly tend to zero as function of R\textsf{R}. In the present paper, the concept is first sharpened for representative models of uncharged fermions moving in external potentials, followed by a discussion of the effects of electron-electron interactions and of perturbing external charges.Comment: final for

    Nearsightedness of Electronic Matter in One Dimension

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    The concept of nearsightedeness of electronic matter (NEM) was introduced by W. Kohn in 1996 as the physical principal underlining Yang's electronic structure alghoritm of divide and conquer. It describes the fact that, for fixed chemical potential, local electronic properties at a point rr, like the density n(r)n(r), depend significantly on the external potential vv only at nearby points. Changes Δv\Delta v of that potential, {\it no matter how large}, beyond a distance R\textsf{R}, have {\it limited} effects on local electronic properties, which tend to zero as function of R\textsf{R}. This remains true even if the changes in the external potential completely surrounds the point rr. NEM can be quantitatively characterized by the nearsightedness range, R(r,Δn)\textsf{\textsf{R}}(r,\Delta n), defined as the smallest distance from rr, beyond which {\it any} change of the external potential produces a density change, at rr, smaller than a given Δn\Delta n. The present paper gives a detailed analysis of NEM for periodic metals and insulators in 1D and includes sharp, explicit estimates of the nearsightedness range. Since NEM involves arbitrary changes of the external potential, strong, even qualitative changes can occur in the system, such as the discretization of energy bands or the complete filling of the insulating gap of an insulator with continuum spectrum. In spite of such drastic changes, we show that Δv\Delta v has only a limited effect on the density, which can be quantified in terms of simple parameters of the unperturbed system.Comment: 10 pages, 9 figure

    Performance Evaluation of a Self-Organising Scheme for Multi-Radio Wireless Mesh Networks

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    Multi-Radio Wireless Mesh Networks (MR-WMN) can substantially increase the aggregate capacity of the Wireless Mesh Networks (WMN) if the channels are assigned to the nodes in an intelligent way so that the overall interference is limited. We propose a generic self-organisation algorithm that addresses the two key challenges of scalability and stability in a WMN. The basic approach is that of a distributed, light-weight, co-operative multiagent system that guarantees scalability. The usefulness of our algorithm is exhibited by the performance evaluation results that are presented for different MR-WMN node densities and typical topologies. In addition, our work complements the Task Group 802.11s Extended Service Set (ESS) Mesh networking project work that is in progress

    Unique Solutions to Hartree-Fock Equations for Closed Shell Atoms

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    In this paper we study the problem of uniqueness of solutions to the Hartree and Hartree-Fock equations of atoms. We show, for example, that the Hartree-Fock ground state of a closed shell atom is unique provided the atomic number ZZ is sufficiently large compared to the number NN of electrons. More specifically, a two-electron atom with atomic number Z≥35Z\geq 35 has a unique Hartree-Fock ground state given by two orbitals with opposite spins and identical spatial wave functions. This statement is wrong for some Z>1Z>1, which exhibits a phase segregation.Comment: 18 page
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