We examine the appearance of superconductivity in the strong-coupling limit of the Hubbard model on the pyrochlore lattice. We focus upon the limit of half-filling, where the normal-state band structure realizes a j=32 semimetal. Introducing doping, we show that the pairing is favored in a J=2 quintet Eg state. The attractive interaction in this channel relies on the fact that Eg pairing on the pyrochlore lattice avoids the detrimental onsite repulsion. Our calculations show that a time-reversal symmetry-breaking superconducting phase is favored, which displays Bogoliubov Fermi surfaces.
Beschreibung
Phys. Rev. B 105, 134507 (2022) - Bogoliubov Fermi surfaces from pairing of emergent $j=\frac{3}{2}$ fermions on the pyrochlore lattice
%0 Journal Article
%1 PhysRevB.105.134507
%A Kobayashi, Shingo
%A Bhattacharya, Ankita
%A Timm, Carsten
%A Brydon, P. M. R.
%D 2022
%I American Physical Society
%J Phys. Rev. B
%K a
%N 13
%P 134507
%R 10.1103/PhysRevB.105.134507
%T Bogoliubov Fermi surfaces from pairing of emergent j=$\dfrac32$ fermions on the pyrochlore lattice
%U https://link.aps.org/doi/10.1103/PhysRevB.105.134507
%V 105
%X We examine the appearance of superconductivity in the strong-coupling limit of the Hubbard model on the pyrochlore lattice. We focus upon the limit of half-filling, where the normal-state band structure realizes a j=32 semimetal. Introducing doping, we show that the pairing is favored in a J=2 quintet Eg state. The attractive interaction in this channel relies on the fact that Eg pairing on the pyrochlore lattice avoids the detrimental onsite repulsion. Our calculations show that a time-reversal symmetry-breaking superconducting phase is favored, which displays Bogoliubov Fermi surfaces.
@article{PhysRevB.105.134507,
abstract = {We examine the appearance of superconductivity in the strong-coupling limit of the Hubbard model on the pyrochlore lattice. We focus upon the limit of half-filling, where the normal-state band structure realizes a j=32 semimetal. Introducing doping, we show that the pairing is favored in a J=2 quintet Eg state. The attractive interaction in this channel relies on the fact that Eg pairing on the pyrochlore lattice avoids the detrimental onsite repulsion. Our calculations show that a time-reversal symmetry-breaking superconducting phase is favored, which displays Bogoliubov Fermi surfaces.},
added-at = {2022-10-20T15:08:12.000+0200},
author = {Kobayashi, Shingo and Bhattacharya, Ankita and Timm, Carsten and Brydon, P. M. R.},
biburl = {https://www.bibsonomy.org/bibtex/22dd213bdd030aea352f568ec876d1d22/ctqmat},
day = 12,
description = {Phys. Rev. B 105, 134507 (2022) - Bogoliubov Fermi surfaces from pairing of emergent $j=\frac{3}{2}$ fermions on the pyrochlore lattice},
doi = {10.1103/PhysRevB.105.134507},
interhash = {8cdcf4814b66ef22e3b2e8c4c2d04e81},
intrahash = {2dd213bdd030aea352f568ec876d1d22},
journal = {Phys. Rev. B},
keywords = {a},
month = {04},
number = 13,
numpages = {15},
pages = 134507,
publisher = {American Physical Society},
timestamp = {2023-10-18T15:11:41.000+0200},
title = {Bogoliubov Fermi surfaces from pairing of emergent j=$\mathbf{\dfrac{3}{2}}$ fermions on the pyrochlore lattice},
url = {https://link.aps.org/doi/10.1103/PhysRevB.105.134507},
volume = 105,
year = 2022
}