Evidence of Andreev bound states as a hallmark of the FFLO phase in $κ$-(BEDT-TTF)$_2$Cu(NCS)$_2$

H. Mayaffre; S. Kramer; M. Horvatić; C. Berthier; K. Miyagawa; K. Kanoda; V. F. Mitrović

doi:10.1038/nphys3121

paper

Evidence of Andreev bound states as a hallmark of the FFLO phase in $κ$ -(BEDT-TTF) $_{2}$ Cu(NCS) $_{2}$

arXiv:1409.0786 · doi:10.1038/nphys3121

Abstract

Superconductivity is a quantum phenomena arising, in its simplest form, from pairing of fermions with opposite spin into a state with zero net momentum. Whether superconductivity can occur in fermionic systems with unequal number of two species distinguished by spin, atomic hyperfine states, flavor, presents an important open question in condensed matter, cold atoms, and quantum chromodynamics, physics. In the former case the imbalance between spin-up and spin-down electrons forming the Cooper pairs is indyced by the magnetic field. Nearly fifty years ago Fulde, Ferrell, Larkin and Ovchinnikov (FFLO) proposed that such imbalanced system can lead to exotic superconductivity in which pairs acquire finite momentum. The finite pair momentum leads to spatially inhomogeneous state consisting of of a periodic alternation of "normal" and "superconducting" regions. Here, we report nuclear magnetic resonance (NMR) measurements providing microscopic evidence for the existence of this new superconducting state through the observation of spin-polarized quasiparticles forming so-called Andreev bound states.

6 pages, 5 figs

Evidence of Andreev bound states as a hallmark of the FFLO phase in $κ$ -(BEDT-TTF) $_{2}$ Cu(NCS) $_{2}$

Abstract

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Cited by in corpus (111)

Evidence of Andreev bound states as a hallmark of the FFLO phase in κ-(BEDT-TTF)2​Cu(NCS)2​

Abstract

References in corpus (14)

Cited by in corpus (111)

Evidence of Andreev bound states as a hallmark of the FFLO phase in $κ$ -(BEDT-TTF) $_{2}$ Cu(NCS) $_{2}$