Field-induced transitions from superconductors to Bose metal in La<sub>1.875</sub>Ba<sub>0.125</sub>CuO<sub>4</sub>

ORAL

Abstract

What happens to the pairing correlations in a cuprate superconductor when superconducting order is suppressed with a magnetic field? We have studied this problem in LBCO x=1/8, where 2D superconductivity appears below 40 K, but 3D order only occurs below 5 K, presumably due to pair-density-wave order intertwined with the spin- and charge-stripe orders. At T = 0.35 K, a c-axis magnetic field initially induces finite dissipation near 10 T, followed by re-entrant 2D superconductivity between 18 and 22 T [1]. The resistance per CuO2 plane rises to h/(4e2) near 31 T, but then saturates at 2h/(4e2) at higher fields. The saturation of the resistance indicates metallic behavior, but the fact that the Hall coefficient is ~ 0 indicates a lack of quasiparticles. We conclude that conduction is by incoherent hopping of pairs between charge stripes, indicating that stripes are good for pairing, but not phase coherence.
[1] Y. Li et al., arXiv:1810.10646.

*Work at BNL supported by Office of Basic Energy Sciences, US DOE, under Contract No. DE-SC0012704. Work at NHMFL and FSU supported by NSF DMR-1707785 and NHMFL via NSF DMR-1644779 and the State of Florida.

Presenters

  • John Tranquada

    • Brookhaven National Laboratory
    • CMPMS, Brookhaven National Laboratory
    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science, Brookhaven National Laboratory
    • Brookhaven Natl Lab

Authors

  • John Tranquada

    • Brookhaven National Laboratory
    • CMPMS, Brookhaven National Laboratory
    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science, Brookhaven National Laboratory
    • Brookhaven Natl Lab
  • Yangmu Li

    • Brookhaven National Laboratory
    • CMPMS, Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science, Brookhaven National Laboratory
  • Genda Gu

    • Brookhaven National Laboratory
    • Brookhaven National Lab
    • Department of Condensed Matter Physics and Materials Science, Brookhaven, Brookhaven National Laboratory, Upton, New York 11973-5000, USA.
    • Cond. Matt. Physics and Material Science, Brookhaven Natl Lab
    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory
    • Brookhaven National Labs, Long Island, NY, USA, 11973
    • Condensed Matter Physics & Materials Science, Brookhaven National Laboratory
    • Condensed Matter Physics, Brookhaven National Laboratory
    • Brookhaven National Laboratories
    • Chinese Academy of Sciences
    • Condensed Matter Physics & Materials Science, Brookhaven National Lab
    • Brookhaven Natl Lab
  • Qiang Li

    • Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science, Brookhaven National Laboratory
  • Alexei Tsvelik

    • Brookhaven National Laboratory
    • CMPMSD, Brookhaven National Laboratory
  • Jasminka Terzic

    • National High Magnetic Field Laboratory
    • National High Magnetic Field Lab
    • Department of Physics and National High Magnetic Field Lab, Florida State University
  • Paul G. Baity

    • Dept. of Phys. & Natl. High Magnetic Field Lab., Florida State Univ.
    • National High Magnetic Field Lab
    • Department of Physics and National High Magnetic Field Lab, Florida State University
    • Dept. of Phys. Natl. High Magnetic Field Lab.
  • Dragana Popovic

    • Dept. of Phys. & Natl. High Magnetic Field Lab., Florida State Univ.
    • National High Magnetic Field Lab
    • Department of Physics and National High Magnetic Field Lab, Florida State University
    • Dept. of Phys. Natl. High Magnetic Field Lab.