Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Ukrainian Mathematical Journal

New second branch of the spectrum of the BCS Hamiltonian and a “pseudogap”

D. Ya. Petrina

Published Nov 1, 2005• 1 citation
Publisher
DOI
10.1007/s11253-006-0028-2

Related papers

Dynamic mean field theory of the Gutzwiller-projected BCS Hamiltonian: phase fluctuation and pseudogap

Kwon Park

Bulletin of the American Physical Society•Mar 6, 2007•0 citations

Spectrum and states of the bcs hamiltonian in a finite domain. I. Spectrum

D. Ya. Petrina

Ukrainian Mathematical Journal•May 1, 2000•7 citations

Spectrum and states of the BCS Hamiltonian with sources

D. Ya. Petrina

Ukrainian Mathematical Journal•Sep 1, 2008•2 citations

Spectrum and States of the BCS Hamiltonian in a Finite Domain. II. Spectra of Excitations

D. Ya. Petrina

Ukrainian Mathematical Journal•Aug 1, 2001•6 citations

Pseudogap phenomena in the BCS pairing model

Satoshi Fujimoto

arXiv:cond-mat/0201380•Physica C Superconductivity•May 1, 2003•0 citations

Interplay of the pseudogap and the BCS gap for heteropairs in 40 K- 6 Li mixture

P. Lipavský, Christophe Berthod

The description of heteropairs like 40 K- 6 Li near and in the superconducting state requires a fully self-consistent theory (see H anai R. and O hashi Y., Phys. Rev. A , 90 (2014) 043622). We derive analytic pseudogap Green's functions for the “normal” and superconducting states from the Luttinger-Ward theory with the T -matrix in the static separable approximation. The self-consistency in the closing loop of self-energy has two pronounced effects on the single-particle spectrum. First, the single-particle excitations decay before the asymptotic quasiparticle propagation is established, therefore the normal state is not a Fermi liquid. Second, the pseudogap has a V shape even for s -wave pairing. The V-shaped pseudogap and the U-shaped BCS gap interfere resulting in slope breaks of the gap walls and the in-gap states in the density of states. Various consequences of an incomplete self-consistency are demonstrated.

arXiv:1609.00240•Europhysics Letters (EPL)•Nov 1, 2016•0 citations
The description of heteropairs like 40 K- 6 Li near and in the superconducting state requires a fully self-consistent theory (see H anai R. and O hashi Y., Phys. Rev. A , 90 (2014) 043622). We derive analytic pseudogap Green's functions for the “normal” and superconducting states from the Luttinger-Ward theory with the T -matrix in the static separable approximation. The self-consistency in the closing loop of self-energy has two pronounced effects on the single-particle spectrum. First, the single-particle excitations decay before the asymptotic quasiparticle propagation is established, therefore the normal state is not a Fermi liquid. Second, the pseudogap has a V shape even for s -wave pairing. The V-shaped pseudogap and the U-shaped BCS gap interfere resulting in slope breaks of the gap walls and the in-gap states in the density of states. Various consequences of an incomplete self-consistency are demonstrated.