Nematic Bogoliubov Fermi surfaces from magnetic toroidal order in FeSeS
arXiv:2306.11200 · doi:10.1103/PhysRevB.109.L220501
Abstract
Recently it has been argued that the superconducting state of FeSeS exhibits Bogoliubov Fermi surfaces for . These Bogoliubov Fermi surfaces appear together with broken time-reversal symmetry and surprisingly demonstrate nematic behavior in a structurally tetragonal phase. Through a symmetry-based analysis of Bogoliubov Fermi surfaces that can arise from broken time-reversal symmetry, we argue that the likely origin of time-reversal symmetry breaking is due to magnetic toroidal order. We show that this magnetic toroidal order naturally appears as a consequence of either static Néel antiferromagnetic order or due to the formation of a spontaneous pair density wave superconducting order. Finally, we reveal that independent of the presence of Bogoliubov Fermi surfaces, supercurrents will induce Néel magnetic order in many Fe-based superconductors.
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Cited by in corpus (4)
- Identifying Bogoliubov Fermi surfaces via thermoelectric response in a -wave superconductor heterostructure
- Spin fluctuations in the ultranodal superconducting state of Fe(Se,S)
- Odd-frequency pairing of Bogoliubov quasiparticles in superconductor junction
- Temperature evolution of the Fermi surface of the FeSe monolayer on SrTiO