Quasiparticle Excitations in the Superconducting State of FeSe Probed by Thermal Hall Conductivity in the Vicinity of the BCS-BEC Crossover
arXiv:1607.03256 · doi:10.7566/JPSJ.86.014707
Abstract
There is growing evidence that the superconducting semimetal FeSe ( K) is in the crossover regime between weak-coupling Bardeen-Cooper-Schrieffer (BCS) and strong-coupling Bose-Einstein-condensate (BEC) limits. We report on longitudinal and transverse thermal conductivities, and , respectively, in magnetic fields up to 20 T. The field dependences of and imply that a highly anisotropic small superconducting gap forms at the electron Fermi-surface pocket whereas a more isotropic and larger gap forms at the hole pocket. Below K, both and exhibit distinct anomalies (kinks) at the upper critical field and at a field slightly below . The analysis of the thermal Hall angle () indicates a change of the quasiparticle scattering rate at . These results provide strong support to the previous suggestion that above a distinct field-induced superconducting phase emerges with an unprecedented large spin imbalance.
arXiv comment7 pages, 3 figures, to be published in JPSJ
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