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Pressure tuning of CeRhIn<sub>5</sub> microstructures

ORAL

Abstract

We revisited the temperature-pressure (Tp) phase diagram of CeRhIn5 utilizing microstructures to probe the electrical resistivity for well-defined crystalline directions along the a- and c-axes of the tetragonal structure. At ambient pressure CeRhIn5 orders antiferromagnetically below 3.8K. Application of external pressure suppresses the antiferromagnetism and induces an unconventional superconducting (SC) state. The Tp phase diagram obtained on the microstructure resembles that of bulk single crystals. Initially, we observe broad SC transitions in resistivity, which sharpen upon approaching the maximum of the SC dome. The electrical resistivity data in the transition region follows the predictions of the Berezinskii-Kosterlitz-Thouless theory proposed for 2D superconductors, e.g. we find the characteristic non-linear I-V curves for current applied along both a- and c- axes. The latter is not expected for CeRhIn5 and puts a purely intrinsic origin of the 2D superconductivity related to 2D antiferromagnetic fluctuations in question. That is supported by finite element analysis of strain-fields in the microstructure. Therefore, we speculate that the observed features of 2D superconductivity in CeRhIn5 may have an origin in a combination of intrinsic and extrinsic effects.

Presenters

  • Janas Kunnelakat John

    Max Planck Institute for Chemical Physics of Solids

Authors

  • Janas Kunnelakat John

    Max Planck Institute for Chemical Physics of Solids

  • Maja Bachmann

    Max Planck Institute for Chemical Physics of Solids, Max Planck Institute for Chemical Physics of Solids, 01187 Dresden

  • Filip Ronning

    Los Alamos National Lab, Los Alamos National Laboratory, Los Alamos National laboratory, Condensed Matter and Magnet Science Group, Los Alamos National Laboratory

  • Eric D Bauer

    Los Alamos National Laboratory, Los Alamos National Lab, Los Alamos National laboratory, Los Alamos Natl Lab, Condensed Matter and Magnet Science Group, Los Alamos National Laboratory, Los Alamos National LAborator

  • Joe Thompson

    Los Alamos National Lab, Los Alamos National laboratory, Los Alamos National Laboratory

  • Philip Moll

    Ecole Polytechnique Federale de Lausanne, Laboratory of Quantum Materials (QMAT), Institute of Materials (IMX), Ecole Polytechnique Federale de Lausanne (EPFL)

  • Michael Nicklas

    Max Planck Institute for Chemical Physics of Solids