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Pseudogap phase of cuprate superconductors confined by Fermi surface topology

  • N. Doiron-Leyraud*
  • , O. Cyr-Choinière
  • , S. Badoux
  • , A. Ataei
  • , C. Collignon
  • , A. Gourgout
  • , S. Dufour-Beauséjour
  • , F. F. Tafti
  • , F. Laliberté
  • , M. E. Boulanger
  • , M. Matusiak
  • , D. Graf
  • , M. Kim
  • , J. S. Zhou
  • , N. Momono
  • , T. Kurosawa
  • , H. Takagi
  • , Louis Taillefer
  • *Corresponding author for this work
  • Université de Sherbrooke
  • Polish Academy of Sciences
  • Florida State University
  • Université Paris-Saclay
  • Collège de France
  • University of Texas at Austin
  • Muroran Institute of Technology
  • Hokkaido University
  • The University of Tokyo
  • Canadian Institute for Advanced Research

Research output: Contribution to journalJournal articlepeer-review

Abstract

The properties of cuprate high-temperature superconductors are largely shaped by competing phases whose nature is often a mystery. Chiefly among them is the pseudogap phase, which sets in at a doping p* that is material-dependent. What determines p* is currently an open question. Here we show that the pseudogap cannot open on an electron-like Fermi surface, and can only exist below the doping pFS at which the large Fermi surface goes from hole-like to electron-like, so that p* ≤ pFS. We derive this result from high-magnetic-field transport measurements in La1.6−xNd0.4SrxCuO4 under pressure, which reveal a large and unexpected shift of p* with pressure, driven by a corresponding shift in pFS. 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.

Original languageEnglish
Article number2044
JournalNature Communications
Volume8
Issue number1
DOIs
StatePublished - 2017.12.1

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