Pressure Effects Show that the Pseudogap Phase of Cuprates is Confined by Fermi Surface Topology

ORAL

Abstract

The pseudogap phase is the central puzzle of cuprate high-temperature superconductors, and why it onsets below a critical doping p* that is much lower in La2−xSrxCuO4 than in La1.6−xNdySrxCuO4 or Bi2Sr2CuO6+δ, for instance, is unknown. We recently performed high-magnetic-field transport measurements in the cuprate La1.6−xNdySrxCuO4 and observed a large and unexpected shift of the pseudogap critical point p* as a function of applied pressure. We find that the shift in p* is driven by a corresponding shift in pFS, the doping at which the large Fermi surface goes from hole-like to electron-like, so that p* ≤ pFS must be obeyed. Consequently, the pseudogap cannot open on an electron-like Fermi surface. This necessary condition for pseudogap formation, imposed by details of the Fermi surface, is a strong constraint for theories of the pseudogap phase. Our finding that p* can be tuned with a modest pressure opens a new route for experimental studies of the pseudogap.

*Work performed in part at the NHMFL. Work funded by NSERC, FRQNT, CFI, and a Canada Research Chair.

Presenters

  • Nicolas Doiron-Leyraud

    • Université de Sherbrooke

Authors

  • Nicolas Doiron-Leyraud

    • Université de Sherbrooke
  • O. Cyr-Choinière

    • Université de Sherbrooke
  • Sven Badoux

    • Institut quantique, University of Sherbrooke
    • Univ of Sherbrooke
    • Université de Sherbrooke
    • University of Sherbrooke
  • Amirreza Ataei

    • Université de Sherbrooke
    • University of Sherbrooke
  • Clement Collignon

    • Institut quantique, University of Sherbrooke
    • Université de Sherbrooke
  • Adrien Gourgout

    • Institut quantique, University of Sherbrooke
    • Université de Sherbrooke
  • Sophie Dufour-Beauséjour

    • Université de Sherbrooke
  • Fazel Tafti

    • Université de Sherbrooke
    • Universite de Sherbrooke
    • Boston College
  • Francis Laliberte

    • Institut quantique, University of Sherbrooke
    • Univ of Sherbrooke
    • Université de Sherbrooke
    • University of Sherbrooke
    • Institut Quantique, Universite de Sherbrooke
  • Marie-Eve Boulanger

    • Université de Sherbrooke
  • Marcin Matusiak

    • Université de Sherbrooke
  • Louis Taillefer

    • Institut quantique, University of Sherbrooke
    • Univ of Sherbrooke
    • Université de Sherbrooke
    • University of Sherbrooke
  • David Graf

    • NHMFL Tallahassee
    • NHMFL
    • National High Magnetic Field Lab
    • National High Magnetic Field Laboratory
    • National High Magnetic Field Laboratory/Florida State University
    • Natl High Magnetic Field Lab
    • NHMFL at Florida State University
    • Florida State University, National High Magnetic Field Laboratory
    • Florida State University
    • Condensed Matter Science, NHMFL
  • Minjae Kim

    • École Polytechnique
    • CNRS, Université Paris-Saclay
    • CPHT, Ecole Polytechnique
  • Jianshi Zhou

    • Univ of Texas
    • University of Texas
    • University of Texas at Austin
    • Texas Materials Institute, University of Texas at Austin
    • Univ of Texas, Austin
    • Mechanical Engineering, University of Texas at Austin
    • University of Texas, at Austin
  • Hidenori Takagi

    • University of Tokyo