Orbital-Free Density Functional Theory: Kinetic Potentials and Ab-Initio Local Pseudopotentials

Details Orbital-Free Density Functional Theory: Kinetic Potentials and Ab-Initio Local Pseudopotentials Orbital-Free Density Functional Theory: Kinetic Potentials and Ab-Initio Local Pseudopotentials

2007-04-14

arxiv.org/abs/0704.1878v1

Physics

Condensed Matter

Strongly Correlated Electrons

To be published in Phys. Rev. B

Scientific paper

10.1103/PhysRevB.75.205122

In the density functional (DF) theory of Kohn and Sham, the kinetic energy of the ground state of a system of noninteracting electrons in a general external field is calculated using a set of orbitals. Orbital free methods attempt to calculate this directly from the electron density by approximating the universal but unknown kinetic energy density functional. However simple local approximations are inaccurate and it has proved very difficult to devise generally accurate nonlocal approximations. We focus instead on the kinetic potential, the functional derivative of the kinetic energy DF, which appears in the Euler equation for the electron density. We argue that the kinetic potential is more local and more amenable to simple physically motivated approximations in many relevant cases, and describe two pathways by which the value of the kinetic energy can be efficiently calculated. We propose two nonlocal orbital free kinetic potentials that reduce to known exact forms for both slowly varying and rapidly varying perturbations and also reproduce exact results for the linear response of the density of the homogeneous system to small perturbations. A simple and systematic approach for generating accurate and weak ab-initio local pseudopotentials which produce a smooth slowly varying valence component of the electron density is proposed for use in orbital free DF calculations of molecules and solids. The use of these local pseudopotentials further minimizes the possible errors from the kinetic potentials. Our theory yields results for the total energies and ionization energies of atoms, and for the shell structure in the atomic radial density profiles that are in very good agreement with calculations using the full Kohn-Sham theory.

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