122 research outputs found
Momentum distribution of the uniform electron gas: improved parametrization and exact limits of the cumulant expansion
The momentum distribution of the unpolarized uniform electron gas in its
Fermi-liquid regime, n(k,r_s), with the momenta k measured in units of the
Fermi wave number k_F and with the density parameter r_s, is constructed with
the help of the convex Kulik function G(x). It is assumed that , the on-top pair density g(0,r_s) and the kinetic energy t(r_s)
are known (respectively, from effective-potential calculations, from the
solution of the Overhauser model, and from Quantum Monte Carlo calculations via
the virial theorem). Information from the high- and the low-density limit,
corresponding to the random-phase approximation and to the Wigner crystal
limit, is used. The result is an accurate parametrization of n(k,r_s), which
fulfills most of the known exact constraints. It is in agreement with the
effective-potential calculation of Takada and Yasuhara [1991 {\it Phys. Rev.} B
{\bf 44} 7879], is compatible with Quantum Monte Carlo data, and is valid in
the density range . The corresponding cumulant expansions of
the pair density and of the static structure factor are discussed, and some
exact limits are derived
Range separation combined with the Overhauser model: Application to the H molecule along the dissociation curve
The combination of density-functional theory with other approaches to the
many-electron problem through the separation of the electron-electron
interaction into a short-range and a long-range contribution (range separation)
is a successful strategy, which is raising more and more interest in recent
years. We focus here on a range-separated method in which only the short-range
correlation energy needs to be approximated, and we model it within the
"extended Overhauser approach". We consider the paradigmatic case of the H
molecule along the dissociation curve, finding encouraging results. By means of
very accurate variational wavefunctions, we also study how the effective
electron-electron interaction appearing in the Overhauser model should be in
order to yield the exact correlation energy for standard Kohn-Sham density
functional theory.Comment: submitted to Int. J. Quantum Chem., special issue dedicated to Prof.
Hira
Study of the discontinuity of the exchange-correlation potential in an exactly soluble case
It was found by Perdew, Parr, Levy, and Balduz [Phys. Rev. Lett. {\bf 49},
1691 (1982)] and by Sham and Schl\"uter [Phys. Rev. Lett. {\bf 51}, 1884
(1983)] that the exact Kohn-Sham exchange-correlation potential of an open
system may jump discontinuosly as the particle number crosses an integer, with
important physical consequences. Recently, Sagvolden and Perdew [Phys. Rev. A
{\bf 77}, 012517 (2008)] have analyzed the discontinuity of the
exchange-correlation potential as the particle number crosses one, with an
illustration that uses a model density for the H ion. In this work, we
extend their analysis to the case in which the external potential is the simple
harmonic confinement, choosing spring-constant values for which the
two-electron hamiltonian has an analytic solution. This way, we can obtain the
exact, analytic, exchange and correlation potentials for particle number
fluctuating between zero and two, illustrating the discontinuity as the
particle number crosses one without introducing any model or approximation. We
also discuss exchange and correlation separately.Comment: Submitted to Int. J. Quantum Chem., special issue honoring Prof.
Mayer. New version, where an important error has been correcte
London dispersion forces without density distortion: a path to first principles inclusion in density functional theory
We analyse a path to construct density functionals for the dispersion
interaction energy from an expression in terms of the ground state densities
and exchange-correlation holes of the isolated fragments. The expression is
based on a constrained search formalism for a supramolecular wavefunction that
is forced to leave the diagonal of the many-body density matrix of each
fragment unchanged, and is exact for the interaction between one-electron
densities. We discuss several aspects: the needed features a density functional
approximation for the exchange-correlation holes of the monomers should have,
the optimal choice of the one-electron basis needed (named "dispersals"), and
the functional derivative with respect to monomer density variations.Comment: 12 pages, 4 figure
Challenging the Lieb-Oxford Bound in a systematic way
The Lieb-Oxford bound, a nontrivial inequality for the indirect part of the
many-body Coulomb repulsion in an electronic system, plays an important role in
the construction of approximations in density functional theory. Using the
wavefunction for strictly-correlated electrons of a given density, we turn the
search over wavefunctions appearing in the original bound into a more
manageable search over electron densities. This allows us to challenge the
bound in a systematic way. We find that a maximizing density for the bound, if
it exists, must have compact support. We also find that, at least for particle
numbers , a uniform density profile is not the most challenging for
the bound. With our construction we improve the bound for electrons that
was originally found by Lieb and Oxford, we give a new lower bound to the
constant appearing in the Lieb-Oxford inequality valid for any , and we
provide an improved upper bound for the low-density uniform electron gas
indirect energy.Comment: accepted in Mol. Phys. in the special issue in honour of Andreas
Savin; revised version with new calculation
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