TY - JOUR
T1 - Evidence for an Fulde-Ferrell-Larkin-Ovchinnikov State with Segmented Vortices in the BCS-BEC-Crossover Superconductor FeSe
AU - Kasahara, S.
AU - Sato, Y.
AU - Licciardello, S.
AU - Čulo, M.
AU - Arsenijević, S.
AU - Ottenbros, T.
AU - Tominaga, T.
AU - Böker, J.
AU - Eremin, I.
AU - Shibauchi, T.
AU - Wosnitza, J.
AU - Hussey, N. E.
AU - Matsuda, Y.
N1 - Funding Information:
We thank M. Houzet, J. S. Kim, and Y. Yanase for stimulating discussion. This work is supported by Grants-in-Aid for Scientific Research (KAKENHI) (Grants No. 15H02106, No. 15H03688, No. 15KK0160, No. 18H01177, No. 18H05227, and No. 19H00649) and on Innovative Areas “Topological Material Science” (No. 15H05852) “Quantum Liquid Crystals” (No. 19H05824) from the Japan Society for the Promotion of Science. We acknowledge support from the Deutsche Forschungsgemeinschaft (DFG) through the Würzburg-Dresden Cluster of Excellence on Complexity and Topology in Quantum Matter ct.qmat (EXC 2147, Project No. 39085490), the ANR-DFG Grant Fermi-NESt, and the former Foundation for Fundamental Research on Matter (FOM), which is financially supported by the Netherlands Organisation for Scientific Research (NWO) (Grant No. 16METL01)—“Strange Metals.” The work of I. E. was also supported by the NUST MISiS Grant No. K2-2017-085 from the Ministry of Science and Higher Education of the Russian Federation in the framework of Increase Competitiveness Program. This work is also supported by the High Field Magnet Laboratory (HFML) at Radboud University (RU) and Hochfeld-Magnetlabor Dresden (HLD) at Helmholtz-Zentrum Dresden-Rossendorf (HZDR), members of the European Magnetic Field Laboratory (EMFL).
Publisher Copyright:
© 2020 American Physical Society.
PY - 2020/3/13
Y1 - 2020/3/13
N2 - We present resistivity and thermal-conductivity measurements of superconducting FeSe in intense magnetic fields up to 35 T applied parallel to the ab plane. At low temperatures, the upper critical field μ0Hc2ab shows an anomalous upturn, while thermal conductivity exhibits a discontinuous jump at μ0H∗≈24 T well below μ0Hc2ab, indicating a first-order phase transition in the superconducting state. This demonstrates the emergence of a distinct field-induced superconducting phase. Moreover, the broad resistive transition at high temperatures abruptly becomes sharp upon entering the high-field phase, indicating a dramatic change of the magnetic-flux properties. We attribute the high-field phase to the Fulde-Ferrel-Larkin-Ovchinnikov (FFLO) state, where the formation of planar nodes gives rise to a segmentation of the flux-line lattice. We point out that strongly orbital-dependent pairing as well as spin-orbit interactions, the multiband nature, and the extremely small Fermi energy are important for the formation of the FFLO state in FeSe.
AB - We present resistivity and thermal-conductivity measurements of superconducting FeSe in intense magnetic fields up to 35 T applied parallel to the ab plane. At low temperatures, the upper critical field μ0Hc2ab shows an anomalous upturn, while thermal conductivity exhibits a discontinuous jump at μ0H∗≈24 T well below μ0Hc2ab, indicating a first-order phase transition in the superconducting state. This demonstrates the emergence of a distinct field-induced superconducting phase. Moreover, the broad resistive transition at high temperatures abruptly becomes sharp upon entering the high-field phase, indicating a dramatic change of the magnetic-flux properties. We attribute the high-field phase to the Fulde-Ferrel-Larkin-Ovchinnikov (FFLO) state, where the formation of planar nodes gives rise to a segmentation of the flux-line lattice. We point out that strongly orbital-dependent pairing as well as spin-orbit interactions, the multiband nature, and the extremely small Fermi energy are important for the formation of the FFLO state in FeSe.
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U2 - 10.1103/PhysRevLett.124.107001
DO - 10.1103/PhysRevLett.124.107001
M3 - Article
C2 - 32216412
AN - SCOPUS:85082561306
SN - 0031-9007
VL - 124
JO - Physical Review Letters
JF - Physical Review Letters
IS - 10
M1 - 107001
ER -