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

Manifestation of the multiband nature in the BCS-BEC crossover of FeSe 1- x S x

Takahiro Hashimoto, Y. Ota, Akihiro Tsuzuki, Tsubaki Nagashima, Akiko Fukushima, S. Kasahara, Yuji Matsuda, Kohei Matsuura, Yuta Mizukami, T. Shibauchi, Shik Shin, Kozo Okazaki

Published Mar 2, 2020• 0 citations
OpenAlex

Related papers

BCS-BEC crossover in FeSe with small Fermi energies

S. Kasahara

Bulletin of the American Physical Society•Mar 16, 2017•0 citations

Preformed pairing in superconducting FeSe in the BCS-BEC cross-over regime

S. Kasahara, Yusuke Shimoyama, Ryota Kobayashi +9 more

Bulletin of the American Physical Society•Mar 2, 2015•0 citations

Thermodynamic quantities in the BCS-BEC crossover region of multiband superconductors

Matsuba Shin'ya, Takeshi Mizushima, Satoshi Fujimoto

日本物理学会講演概要集•Jan 1, 2020•0 citations

Evidence for FFLO superconducting states in the BCS-BEC crossover superconductor FeSe

S. Kasahara

Bulletin of the American Physical Society•Mar 18, 2021•0 citations

Superconductivity of the FeSe/SrTiO3 Interface in View of BCS–BEC Crossover*

Shuyuan Zhang, Guangyao Miao, Jiaqi Guan +6 more

In paired Fermi systems, strong many-body effects exhibit in the crossover regime between the Bardeen–Cooper–Schrieffer (BCS) and the Bose–Einstein condensation (BEC) limits. The concept of the BCS–BEC crossover, which is studied intensively in the research field of cold atoms, has been extended to condensed matters. Here by analyzing the typical superconductors within the BCS–BEC phase diagram, we find that FeSe-based superconductors are prone to shift their positions in the BCS–BEC crossover regime by charge doping or substrate substitution, since their Fermi energies and the superconducting gap sizes are comparable. Especially at the interface of single-layer FeSe on SrTiO 3 substrate, the superconductivity is relocated closer to the crossover unitary than other doped FeSe-based materials, indicating that the pairing interaction is effectively modulated. We further show that hole-doping can drive the interfacial system into the phase with possible pre-paired electrons, demonstrating its flexible tunability within the BCS–BEC crossover regime.

arXiv:1908.11126•Chinese Physics Letters•Oct 1, 2019•9 citations

Hidden Pseudogap and Excitation Spectra in a Strongly Coupled Two-Band Superfluid/Superconductor

Hiroyuki Tajima, Pierbiagio Pieri, Andrea Perali

We investigate single-particle excitation properties in the normal state of a two-band superconductor or superfluid throughout the Bardeen–Cooper–Schrieffer (BCS) to Bose–Einstein-condensation (BEC) crossover, within the many-body T-matrix approximation for multichannel pairing fluctuations. We address the single-particle density of states and the spectral functions consisting of two contributions associated with a weakly interacting deep band and a strongly interacting shallow band, relevant for iron-based multiband superconductors and multicomponent fermionic superfluids. We show how the pseudogap state in the shallow band is hidden by the deep band contribution throughout the two-band BCS-BEC crossover. Our results could explain the missing pseudogap in recent scanning tunneling microscopy experiments in FeSe superconductors.

arXiv:2012.12647•Condensed Matter•Feb 7, 2021•2 citations
In paired Fermi systems, strong many-body effects exhibit in the crossover regime between the Bardeen–Cooper–Schrieffer (BCS) and the Bose–Einstein condensation (BEC) limits. The concept of the BCS–BEC crossover, which is studied intensively in the research field of cold atoms, has been extended to condensed matters. Here by analyzing the typical superconductors within the BCS–BEC phase diagram, we find that FeSe-based superconductors are prone to shift their positions in the BCS–BEC crossover regime by charge doping or substrate substitution, since their Fermi energies and the superconducting gap sizes are comparable. Especially at the interface of single-layer FeSe on SrTiO 3 substrate, the superconductivity is relocated closer to the crossover unitary than other doped FeSe-based materials, indicating that the pairing interaction is effectively modulated. We further show that hole-doping can drive the interfacial system into the phase with possible pre-paired electrons, demonstrating its flexible tunability within the BCS–BEC crossover regime.
We investigate single-particle excitation properties in the normal state of a two-band superconductor or superfluid throughout the Bardeen–Cooper–Schrieffer (BCS) to Bose–Einstein-condensation (BEC) crossover, within the many-body T-matrix approximation for multichannel pairing fluctuations. We address the single-particle density of states and the spectral functions consisting of two contributions associated with a weakly interacting deep band and a strongly interacting shallow band, relevant for iron-based multiband superconductors and multicomponent fermionic superfluids. We show how the pseudogap state in the shallow band is hidden by the deep band contribution throughout the two-band BCS-BEC crossover. Our results could explain the missing pseudogap in recent scanning tunneling microscopy experiments in FeSe superconductors.