https://doi.org/10.1007/s100510051019
Superconductivity in weakly correlated electron systems
Institut für Theoretische Physik, Universtät Bremen,
Postfach 330 440, 28 334 Bremen, Germany
Corresponding author: a czycholl@theo.physik.uni-bremen.de
Received:
17
February
1999
Published online: 15 December 1999
We study the influence of the short-ranged Hubbard correlation U between
the conduction electrons on the Cooper pair formation in normal (s-wave)
superconductors. The Coulomb correlation is considered within the standard
second order perturbation theory, which becomes exact in the weak
coupling limit but goes beyond the simple Hartree-Fock treatment by
yielding a finite lifetime of the quasiparticles
at finite temperature. An attractive pairing interaction V, which may be
mediated by the standard electron-phonon mechanism, is considered between
nearest neighbor sites.
A critical value Vc for the attractive interaction is
required to obtain a superconducting state. For finite temperature
a gapless superconductivity is obtained due to the finite lifetime of the
quasiparticles, i.e. the Coulomb correlation has a pair-breaking influence.
The energy gap Δ and Tc depend
very sensitively on U, V and band filling n and develop a maximum
away from half filling as function of n. The ratio
varies with n, being higher than the BCS value near half filling
and reaching the BCS value for lower n.
PACS: 74.20.Fg – BCS theory and its development / 71.27.+a – Strongly correlated electron systems; heavy fermions / 71.10.-w – Theories and models of many electron systems
© EDP Sciences, Società Italiana di Fisica, Springer-Verlag, 1999