Bogoliubov Fermi surfaces in the superconducting state of tetragonal FeSe<sub>1-x</sub>S<sub>x</sub>
ORAL · Invited
Abstract
Recently, topologically protected ultranodal pairing states with so-called Bogoliubov Fermi surfaces have been predicted in time-reversal symmetry-breaking (TRSB) superconductors [1,2]. The iron-chalcogenide superconductors FeSe1-xSx are among the most promising candidates for such exotic superconducting states. In FeSe1-xSx, nematic order (tetragonal-to-orthogonal structural transition) can be completely suppressed at x = 0.17, above which the superconducting properties change drastically and the residual density of states in the superconducting state is significantly enhanced [3-5]. Our recent muon spin rotation (μSR) measurements reveal that TRSB occurs just below the superconducting transition temperature and a significant fraction of electrons remains unpaired in the superconducting state of the tetragonal phase [6]. These results are consistent with the ultranodal pairing state with BFSs. I will review recent studies of FeSe1-xSx superconductors, showing exotic superconducting states, including recent direct observations of BFSs in angle-resolved photoemission spectroscopy (ARPES) measurements [7] and a strong upturn of the nuclear magnetic relaxation (NMR) rate in the superconducting state associated with possible nesting properties between BFSs [8] as well as a possible impurity-induced disappearance of BFSs revealed by penetration depth measurements in the tetragonal FeSe1-xSx [9].
[1] D. F. Agterberg, P. M. R. Brydon, and C. Timm, Phys. Rev. Lett. 118, 127001 (2017).
[2] C. Setty et al, Nat. Commun. 11, 523 (2020).
[3] Y. Sato et al., Proc. Natl. Acad. Sci. USA 115, 1227 (2018).
[4] T. Hanaguri et al., Sci. Adv. 4, eaar6419 (2018).
[5] Y. Mizukami et al., Commun. Phys. 6, 183 (2023).
[6] K. Matsuura et al., Proc. Natl. Acad. Sci. USA 120, e2208276120 (2023).
[7] T. Nagashima, T. Hashimoto et al., preprint (2023).
[8] Z.-Y. Yu et al., Commun. Phys. 6, 175 (2023).
[9] T. Nagashima, K. Ishihara et al., preprint (2023).
[1] D. F. Agterberg, P. M. R. Brydon, and C. Timm, Phys. Rev. Lett. 118, 127001 (2017).
[2] C. Setty et al, Nat. Commun. 11, 523 (2020).
[3] Y. Sato et al., Proc. Natl. Acad. Sci. USA 115, 1227 (2018).
[4] T. Hanaguri et al., Sci. Adv. 4, eaar6419 (2018).
[5] Y. Mizukami et al., Commun. Phys. 6, 183 (2023).
[6] K. Matsuura et al., Proc. Natl. Acad. Sci. USA 120, e2208276120 (2023).
[7] T. Nagashima, T. Hashimoto et al., preprint (2023).
[8] Z.-Y. Yu et al., Commun. Phys. 6, 175 (2023).
[9] T. Nagashima, K. Ishihara et al., preprint (2023).
*This work was supported mainly by Grant-in-Aid for Scientific Research on innovative areas "Quantum Liquid Crystals" (No. JP19H05824) and Grant-in-Aid for Scientific Research for Transformative Research Areas (A) "Condensed Conjugation" (No. JP20H05869) from Japan Society for the Promotion of Science (JSPS).
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Publication: K. Matsuura et al., Proc. Natl. Acad. Sci. USA 120, e2208276120 (2023).
T. Nagashima, T. Hashimoto et al., preprint (2023).
T. Nagashima, K. Ishihara et al., preprint (2023).
Presenters
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Kenichiro Hashimoto
- The University of Tokyo
- Dept. of Adv. Mater. Sci., Univ. of Tokyo
- U. Tokyo
- Univ. of Tokyo
- University of Tokyo