This paper deals with the ground state of an interacting electron
gas in an external potential v(r). It is proved that there exists
a universal functional of the density, Fn(r), independent of v(r),
such that the expression E??v(r)n(r)dr+Fn(r) has as its minimum
value the correct ground-state energy associated with v(r). The functional
Fn(r) is then discussed for two situations: (1) n(r)=n0+n?(r),
n?/n0?1, and (2) n(r)=?(r/r0) with ? arbitrary and r0??. In both
cases F can be expressed entirely in terms of the correlation energy
and linear and higher order electronic polarizabilities of a uniform
electron gas. This approach also sheds some light on generalized
Thomas-Fermi methods and their limitations. Some new extensions of
these methods are presented.
%0 Journal Article
%1 Hohenberg1964
%A Hohenberg, P.
%A Kohn, W.
%D 1964
%J Phys. Rev.
%K imported
%N 3B
%P B864-B871
%R 10.1103/PhysRev.136.B864
%T Inhomogeneous Electron Gas
%U ttp://link.aps.org/abstract/PR/v136/pB864
%V 136
%X This paper deals with the ground state of an interacting electron
gas in an external potential v(r). It is proved that there exists
a universal functional of the density, Fn(r), independent of v(r),
such that the expression E??v(r)n(r)dr+Fn(r) has as its minimum
value the correct ground-state energy associated with v(r). The functional
Fn(r) is then discussed for two situations: (1) n(r)=n0+n?(r),
n?/n0?1, and (2) n(r)=?(r/r0) with ? arbitrary and r0??. In both
cases F can be expressed entirely in terms of the correlation energy
and linear and higher order electronic polarizabilities of a uniform
electron gas. This approach also sheds some light on generalized
Thomas-Fermi methods and their limitations. Some new extensions of
these methods are presented.
@article{Hohenberg1964,
abstract = {This paper deals with the ground state of an interacting electron
gas in an external potential v(r). It is proved that there exists
a universal functional of the density, F[n(r)], independent of v(r),
such that the expression E??v(r)n(r)dr+F[n(r)] has as its minimum
value the correct ground-state energy associated with v(r). The functional
F[n(r)] is then discussed for two situations: (1) n(r)=n0+n?(r),
n?/n0?1, and (2) n(r)=?(r/r0) with ? arbitrary and r0??. In both
cases F can be expressed entirely in terms of the correlation energy
and linear and higher order electronic polarizabilities of a uniform
electron gas. This approach also sheds some light on generalized
Thomas-Fermi methods and their limitations. Some new extensions of
these methods are presented.},
added-at = {2009-09-09T17:55:18.000+0200},
author = {Hohenberg, P. and Kohn, W.},
biburl = {https://www.bibsonomy.org/bibtex/29089ce780b34295a3aeeef9d6875cda4/pbuczek},
doi = {10.1103/PhysRev.136.B864},
file = {Hohenberg1964.pdf:Hohenberg1964.pdf:PDF;Hohenberg1964.pdf:Hohenberg1964.pdf:PDF},
interhash = {768a46ec6e3e56a9ab77cc01695db5d6},
intrahash = {9089ce780b34295a3aeeef9d6875cda4},
journal = {Phys. Rev.},
keywords = {imported},
month = {November },
number = {3B },
owner = {pbuczek},
pages = {B864-B871},
timestamp = {2009-09-09T17:55:35.000+0200},
title = {Inhomogeneous Electron Gas},
url = {ttp://link.aps.org/abstract/PR/v136/pB864},
volume = 136,
year = 1964
}