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

Bulletin of the American Physical Society

The spectral function of the normal phase in the BCS-BEC crossover

Tara E. Drake, Yoav Sagi, Rabin Paudel, Roman Chapurin, Deborah Jin

Published Jun 11, 2015• 0 citations
OpenAlex

Related papers

Normal state spin susceptibility in the BEC-BCS crossover region.

Yun Long, Feng Xiong, Colin Parker

Bulletin of the American Physical Society•Jun 3, 2020•0 citations

BCS-BEC crossover at finite temperature in the broken-symmetry phase

P. Pieri, L. Pisani, Giancarlo Calvanese Strinati

The BCS-BEC crossover is studied in a systematic way in the broken-symmetry phase between zero temperature and the critical temperature. This study bridges two regimes where quantum and thermal fluctuations are, respectively, important. The theory is implemented on physical grounds, by adopting a fermionic self-energy in the broken-symmetry phase that represents fermions coupled to superconducting fluctuations in weak coupling and to bosons described by the Bogoliubov theory in strong coupling. This extension of the theory beyond mean field proves important at finite temperature, to connect with the results in the normal phase. The order parameter, the chemical potential, and the single-particle spectral function are calculated numerically for a wide range of coupling and temperature. This enables us to assess the quantitative importance of superconducting fluctuations in the broken-symmetry phase over the whole BCS-BEC crossover. Our results are relevant to the possible realizations of this crossover with high-temperature cuprate superconductors and with ultracold fermionic atoms in a trap.

arXiv:cond-mat/0406099•Physical Review B•Sep 17, 2004•136 citations

Universality and novel phases in the BCS-BEC crossover

W. Zwerger

Bulletin of the American Physical Society•Jun 8, 2007•0 citations

BCS to Bose-Einstein crossover at finite temperature in the broken-symmetry phase

P. Pieri, L. Pisani, Giancarlo Strinati Calvanese

The BCS-BEC crossover is studied in a systematic way in the broken-symmetry phase between zero temperature\nand the critical temperature. This study bridges two regimes where quantum and thermal fluctuations\nare, respectively, important. The theory is implemented on physical grounds, by adopting a fermionic selfenergy\nin the broken-symmetry phase that represents fermions coupled to superconducting fluctuations in weak\ncoupling and to bosons described by the Bogoliubov theory in strong coupling. This extension of the theory\nbeyond mean field proves important at finite temperature, to connect with the results in the normal phase. The\norder parameter, the chemical potential, and the single-particle spectral function are calculated numerically for\na wide range of coupling and temperature. This enables us to assess the quantitative importance of superconducting\nfluctuations in the broken-symmetry phase over the whole BCS-BEC crossover. Our results are relevant\nto the possible realizations of this crossover with high-temperature cuprate superconductors and with\nultracold fermionic atoms in a trap.

Physical Review B•Jan 1, 2004•0 citations

An exactly solvable model of the BCS-BEC crossover

Jean-Noël Fuchs, RECATI A, W. Zwerger

•Jan 1, 2004•0 citations

Potential-energy-driven (BCS) to kinetic-energy-driven (BEC) pairing in the two-dimensional attractive Hubbard model: Cellular dynamical mean-field theory

Bumsoo Kyung, Antoine Georges, A.–M. S. Tremblay

The BCS-BEC crossover within the two-dimensional attractive Hubbard model is studied by using the Cellular Dynamical Mean-Field Theory, both in the normal and superconducting ground states. Short-range spatial correlations incorporated in this theory remove the normal-state quasiparticle peak and the first-order transition found in the Dynamical Mean-Field Theory, rendering the normal state crossover smooth. For $U$ smaller than the bandwidth, pairing is driven by the potential energy, while in the opposite case it is driven by the kinetic energy, resembling a recent optical conductivity experiment in cuprates. Phase coherence leads to the appearance of a collective Bogoliubov mode in the density-density correlation function and to the sharpening of the spectral function.

arXiv:cond-mat/0508645•Physical Review B•Jul 5, 2006•34 citations
The BCS-BEC crossover is studied in a systematic way in the broken-symmetry phase between zero temperature and the critical temperature. This study bridges two regimes where quantum and thermal fluctuations are, respectively, important. The theory is implemented on physical grounds, by adopting a fermionic self-energy in the broken-symmetry phase that represents fermions coupled to superconducting fluctuations in weak coupling and to bosons described by the Bogoliubov theory in strong coupling. This extension of the theory beyond mean field proves important at finite temperature, to connect with the results in the normal phase. The order parameter, the chemical potential, and the single-particle spectral function are calculated numerically for a wide range of coupling and temperature. This enables us to assess the quantitative importance of superconducting fluctuations in the broken-symmetry phase over the whole BCS-BEC crossover. Our results are relevant to the possible realizations of this crossover with high-temperature cuprate superconductors and with ultracold fermionic atoms in a trap.
The BCS-BEC crossover is studied in a systematic way in the broken-symmetry phase between zero temperature\nand the critical temperature. This study bridges two regimes where quantum and thermal fluctuations\nare, respectively, important. The theory is implemented on physical grounds, by adopting a fermionic selfenergy\nin the broken-symmetry phase that represents fermions coupled to superconducting fluctuations in weak\ncoupling and to bosons described by the Bogoliubov theory in strong coupling. This extension of the theory\nbeyond mean field proves important at finite temperature, to connect with the results in the normal phase. The\norder parameter, the chemical potential, and the single-particle spectral function are calculated numerically for\na wide range of coupling and temperature. This enables us to assess the quantitative importance of superconducting\nfluctuations in the broken-symmetry phase over the whole BCS-BEC crossover. Our results are relevant\nto the possible realizations of this crossover with high-temperature cuprate superconductors and with\nultracold fermionic atoms in a trap.
The BCS-BEC crossover within the two-dimensional attractive Hubbard model is studied by using the Cellular Dynamical Mean-Field Theory, both in the normal and superconducting ground states. Short-range spatial correlations incorporated in this theory remove the normal-state quasiparticle peak and the first-order transition found in the Dynamical Mean-Field Theory, rendering the normal state crossover smooth. For UUU smaller than the bandwidth, pairing is driven by the potential energy, while in the opposite case it is driven by the kinetic energy, resembling a recent optical conductivity experiment in cuprates. Phase coherence leads to the appearance of a collective Bogoliubov mode in the density-density correlation function and to the sharpening of the spectral function.