Fermiology of the low carrier density superconductor Tl-doped PbTe, and its non-superconducting analog, Na-doped PbTe.

ORAL

Abstract

PbTe is a narrow band gap semiconductor, which can be electron- or hole-doped, obtaining typical carrier densities of the order of 1x10$^{20}$cm$^{-3}$. The only impurity known to produce superconductivity in this host material is Tl, resulting in a maximum critical temperature of 1.5K - an order of magnitude higher that the T$_{c}$ observed in similar low carrier density semiconductors. In this work we performed a full Fermi surface characterization of Pb$_{1-x}$Tl$_{x}$Te, as well as its non-superconducting analog, Pb$_{1-x}$Na$_{x}$Te, via Shubnikov de Haas oscillations in magnetotransport, for magnetic fields up to 35T (DC). Our results show that beyond a critical impurity concentration close to the emergence of superconductivity, there are clear differences in the normal-state carriers. In non-superconducting Pb$_{1-x}$Na$_{x}$Te, all carriers reside at four ellipsoidal pockets of the Fermi surface, while in superconducting Pb$_{1-x}$Tl$_{x}$Te, there is an additional set of carriers, consistent with incoherent resonant impurity levels. The presence or absence of these states at or near the Fermi energy is intimately connected to the presence or absence of superconductivity in doped PbTe.

Authors

  • Paula Giraldo-Gallo

    Stanford University and National High Magnetic Field Laboratory, National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL, USA

  • Phillip Walmsley

    Stanford University, Stanford

  • Boris Sangiorgio

    Materials Theory, ETH Zurich, ETH Zurich

  • Michael Fechner

    Materials Theory, ETH Zurich, Wolfgang-Pauli-Strasse 27, 8093 Zurich, ETH Zurich

  • Lisa Buchauer

    ESPCI, Paris, France

  • Benoit Fauqué

    LPEM (UPMC-CNRS), Ecole Supérieure de Physique et de Chimie Industrielles, 75005 Paris, France, ESPCI, Paris, France, ESPCI

  • Scott C. Riggs

    NHMFL-FSU, National High Magnetic Field Laboratory, National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL, USA, NHMFL

  • Ross McDonald

    Los Alamos National Laboratory, Los Alamos, NM 87545, USA, LANL, Los Alamos National Laboratory, National High MagneticField Laboratory, Los Alamos National Laboratory, Los Alamos, NM, USA.

  • Theodore Geballe

    Stanford University

  • Nicola Spaldin

    ETH Zurich, Materials Theory, ETH Zurich

  • Kamran Behnia

    LPEM (UPMC-CNRS), Ecole Supérieure de Physique et de Chimie Industrielles, 75005 Paris, France, ESPCI, Paris, France, ESPCI

  • Ian R. Fisher

    Department of Applied Physics and Geballe Laboratory for Advanced Materials Stanford University, Stanford University, Stanford