Phase separation at the dimer-superconductor transition in Ir<sub>1−x</sub>Rh<sub>x</sub>Te<sub>2</sub>

ORAL

Abstract

The detailed evolution of the local atomic structure across the (x, T) phase diagram of Ir1−xRhxTe2 superconductor (0≤x≤0.3, 10K≤T≤300K) is obtained from high-quality x-ray total scattering data using the atomic pair distribution function method. The observed hysteretic thermal structural phase transition from a trigonal to a triclinic dimer phase for low Rh content emphasizes the intimate connection between the lattice and electronic properties. For superconducting samples away from the dimer/superconductor boundary, structural transition is absent and the local structure remains trigonal down to 10 K. In the narrow range of compositions close to the boundary structural phase separation is observed, suggestive of weak first-order character of the Rh-doping induced dimer-superconductor quantum phase transition. Samples from this narrow range show weak anomalies in electronic transport and magnetization, hallmarks of the dimer phase, as well as superconductivity albeit with incomplete diamagnetic screening. The results imply competition of the dimer and superconducting orders.
[1] R. Yu et al., Phys. Rev. B 98, 134506 (2018).
[2] ] R. Yu et al., Phys. Rev. B 97, 174515 (2018).

*Work at Brookhaven National Laboratory was supported by US DOE-BES under Contract No. DE-SC0012704.

Presenters

  • Emil Bozin

    • Brookhaven National Laboratory
    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory

Authors

  • Runze Yu

    • Brookhaven National Laboratory
  • Soham Banerjee

    • Brookhaven National Laboratory
    • Columbia University
  • Hechang Lei

    • Physics Department, Renmin University of China
    • Brookhaven National Laboratory
    • Renmin University of China
    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory
  • Milinda Abeykoon

    • Brookhaven National Laboratory
    • CMPMSD, Brookhaven National Laboratory
  • Cedomir Petrovic

    • CMPMS, Brookhaven National Laboratory
    • Brookhaven National Laboratory
    • CMPMSD, Brookhaven National Laboratory
    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory
  • Zurab Guguchia

    • Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute
    • Paul Scherrer Institut
    • Princeton University
    • Columbia University
    • Brookhaven National Laboratory
  • Emil Bozin

    • Brookhaven National Laboratory
    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory