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Daniel Joubert

Publications and source records attributed to Daniel Joubert.

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Exact Kohn-Sham Density Functional Theory on a Lattice

We formulate a set of equations that facilitate an exact numerical solution of the Kohn-Sham potential for a finite Hubbard chain with nearest neighbour hopping and arbitrary site potentials. The approach relies on a mapping of the non-interacting Kohn-Sham ground state wave function onto the exact interacting system wavefunction and two interconnected self-consistent cycles. The self-consistent cycles are performed within the framework of the Kohn-Sham non-interacting system without any direct reference to the interacting system. The first self-consistent cycle updates the mapping of the non-interacting wavefunction onto the interacting wavefunction based on a trial input density, while the second self-consistent cycle updates the Kohn-Sham potential to yield the trial density. At the solution point, the exact density, the exact Kohn-Sham potential, the density functional correlation energy and the exact interacting system ground state energy are available.

cond-mat.str-el

Convexity and translational invariance constraint on the exchange-correlation functional

Knowledge of the properties of the exchange-correlation functional in the form $\frac 1λv_{xc}([ρ_λ],\frac{\bf r}λ)$, where $ρ_λ({\bf r})=$ $λ^3ρ(λ{\bf r}),$ is important when expressing the exchange-correlation energy as a line integral $% E_{xc}[ρ]=\int_0^1dλ\int d{\bf r}\frac 1λv_{xc}([ρ_λ],\frac{\bf r}λ)\left[ 3ρ({\bf r})+{\bf r.\nabla }ρ({\bf r})\right] $ (van Leeuwen and Baerends, Phys. Rev. A {\bf 51}, 170 (1995)). With this in mind, it is shown that in the low density limit $% \lim_{λ\rightarrow 0}\int ρ({\bf r})\nabla ^2\frac 1λv_{xc}([ρ_λ],\frac{\bf r}λ)\ d^3r\leq 4π\int ρ(% {\bf r})^2d^3r.$ This inequality is violated in the local-density approximation.

cond-mat