Martensitic Transition in the A15 Superconductor Ti<sub>3</sub>Ir

ORAL

Abstract

Transport, thermodynamic, XRD and high-pressure measurements on high-quality Ti3Ir samples reveal a phase transition around T* = 90 K which we identify as a Martensitic transition leading from the cubic to a tetragonal structure with c/a <1. Next to V3Si and Nb3Sn1-xSbx, Ti3Ir is only the third material among all the A15 superconductors displaying a clearly resolved martensitic transition at a unprecedently high temperature. With the application of high pressure, Tc increases while T* decreases. Thus, Ti3Ir does not follow the correlation between pressure derivatives and tetragonal distortion seen for Nb3Sn and V3Si. Furthermore, with pressure the resistivity decreases at temperatures above T* while below it is essentially pressure independent. We attribute this unusual behavior to the strong, pressure dependent coupling between electrons and a G3 optical phonon. Above T*, pressure induced stiffening of the G3 phonon reduces the electron-phonon coupling and the resistivity. Below T*, this phonon freezes out causing the dimerization along the Ti-chains, a concomitant reduction of the over-all resistivity and the removal of the source of pressure dependence.

*This work was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division. XRD was performed at the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science user facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357, and at the Center for High-Energy X-ray Sciences (CHEXS), supported by NSF award DMR-2342336.

Presenters

  • Ulrich Welp

    • Argonne National Laboratory

Authors

  • Ulrich Welp

    • Argonne National Laboratory
  • Ramakanta Chapai

    • Norfolk State University
  • Hengdi Zhao

    • Argonne National Laboratory
    • University of Colorado at Boulder
    • Univeristy of Colorado at Boulder
  • Yu Zhang

    • Argonne National Laboratory
    • Argon National Lab
    • Argonne National Laboratoy
  • Matt P Smylie

    • Hofstra University
  • Pedro Mercado Lozano

    • Argonne National Laboratory, Advanced Photon Source
    • Argonne National Laboratory
  • Hyowon Park

    • University of Illinois at Chicago
  • Duck Young Chung

    • Argonne National Laboratory
  • Stephan Rosenkranz

    • Argonne National Laboratory
  • Philip Ryan

    • Argonne National Laboratory
  • Daniel Phelan

    • Argonne National Laboratory
    • Materials Science Division, Argonne National Laboratory, Lemont, IL 60439, USA
  • John F Mitchell

    • Argonne National Laboratory