2008 APS March Meeting
Volume 53, Number 2
Monday–Friday, March 10–14, 2008;
New Orleans, Louisiana
Session D1: Fundamental Developments in Density Functional Theory
2:30 PM–5:30 PM,
Monday, March 10, 2008
Morial Convention Center
Room: LaLouisiane AB
Sponsoring
Unit:
DCOMP
Chair: Neepa Maitra, Hunter College of the City University of New York
Abstract ID: BAPS.2008.MAR.D1.2
Abstract: D1.00002 : Density-functional theory of superconductivity*
3:06 PM–3:42 PM
Preview Abstract
Abstract
Author:
E.K.U. Gross
(Freie Universitat Berlin)
A prominent challenge of modern condensed-matter theory is to
predict
reliably material-specific properties of superconductors, such as
the
critical temperature. The traditional model of Bardeen, Cooper and
Schrieffer (BCS) properly describes the universal features that all
conventional superconductors have in common, but it is not able
to make
accurate predictions of material-specific properties. To tackle this
problem, a density-functional formalism has been developed [1] which
describes superconductors in thermal equilibrium in terms of three
quantities: the ordinary density, the superconducting order
parameter, and
the nuclear N-body density. These three ``densities'' are determined
self-consistently through a set of Kohn-Sham equations.
Approximations of
the universal exchange-correlation functional are derived on the
basis of
many-body perturbation theory. In this way, a true ab-initio
description is
achieved which does not contain any adjustable parameters such as
the $\mu
$* of Eliashberg theory. Numerical results for the critical
temperature, the
isotope effect, the gap function and the jump of the specific
heat will be
presented for simple metals, for MgB$_{2 }$[2] and CaBeSi, and
for calcium
intercalated graphite (CaC$_{6})$ [3]. Furthermore, results for Li,
Al, K, and H
under pressure will be discussed. The calculations explain why Li
and Al
behave very differently, leading to a strong enhancement of
superconductivity for Li and to a clear suppression for Al with
increasing
pressure [4]. For K we predict a behavior similar to Li, i.e. a
strong
increase of T$_{c}$ with increasing pressure. Finally, hydrogen
is found to be a three-gap superconductor whose critical temperature
increases with increasing pressure until about 100K (at 500 GPa).
\\ \noindent [1] M. L\"{u}ders, M.A.L. Marques, N.N. Lathiotakis,
A. Floris,G. Profeta,
L. Fast, A.Continenza, S. Massidda, E.K.U. Gross, PRB \underline
{\textbf{72}}, 024545 (2005). \\ \noindent [2] A. Floris, G.
Profeta, N.N. Lathiotakis, M. L\"{u}ders, M.A.L. Marques,
C. Franchini, E.K.U. Gross, A. Continenza, S. Massidda, PRL
\underline
{\textbf{94}}, 037004 (2005). \\ \noindent [3] A. Sanna, G.
Profeta, A. Floris, A. Marini, E.K.U. Gross, S. Massidda, PRB
(Rapid Comm.) \underline {\textbf{75}}, 020511 (2007). \\
\noindent [4] G. Profeta, C. Franchini, N.N. Lathiotakis, A.
Floris, A.
Sanna, M.A.L.
Marques, M. L\"{u}ders, S. Massidda, E.K.U. Gross, A. Continenza,
PRL \underline {\textbf{96}}, 047003 (2006).
*In collaboration with A. Floris, G. Profeta, A. Sanna, C. Bersier, N.N. Lathiotakis, M. L\"uders, M.A.L. Marques, C. Franchini, A. Continenza, and S. Massidda.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2008.MAR.D1.2