Observation of strong electron pairing on bands without Fermi surfaces in LiFe1−xCoxAs
H. Miao,
T. Qian (),
X. Shi,
P. Richard,
T. K. Kim,
M. Hoesch,
L. Y. Xing,
X.-C. Wang,
C.-Q. Jin,
J.-P. Hu and
H. Ding ()
Additional contact information
H. Miao: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
T. Qian: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
X. Shi: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
P. Richard: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
T. K. Kim: Diamond Light Source, Harwell Campus
M. Hoesch: Diamond Light Source, Harwell Campus
L. Y. Xing: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
X.-C. Wang: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
C.-Q. Jin: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
J.-P. Hu: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
H. Ding: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
Nature Communications, 2015, vol. 6, issue 1, 1-6
Abstract:
Abstract In conventional BCS superconductors, the quantum condensation of superconducting electron pairs is understood as a Fermi surface instability, in which the low-energy electrons are paired by attractive interactions. Whether this explanation is still valid in high-Tc superconductors such as cuprates and iron-based superconductors remains an open question. In particular, a fundamentally different picture of the electron pairs, which are believed to be formed locally by repulsive interactions, may prevail. Here we report a high-resolution angle-resolved photoemission spectroscopy study on LiFe1−xCoxAs. We reveal a large and robust superconducting gap on a band sinking below the Fermi level on Co substitution. The observed Fermi-surface-free superconducting order is also the largest over the momentum space, which rules out a proximity effect origin and indicates that the order parameter is not tied to the Fermi surface as a result of a surface instability.
Date: 2015
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Persistent link: https://EconPapers.repec.org/RePEc:nat:natcom:v:6:y:2015:i:1:d:10.1038_ncomms7056
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DOI: 10.1038/ncomms7056
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