Electronic in-plane symmetry breaking at field-tuned quantum criticality in CeRhIn5

Invited

Abstract

At the heart of the heavy-fermion problem is the interaction between f-electrons and the itinerant electronic system. Their character may be best described in localized or itinerant pictures, depending on the Kondo- and RKKY-interactions. CeRhIn5 falls in the localized category, and antiferromagnetism appears at TN~3.8K. Applying pressure increases the hybridization, and thus magnetism is suppressed in favor of superconductivity. Magnetic fields are another important parameter tuning the 4f-waveform, and recently a peculiar transition at H*~28T into a new phase emerging in vicinity of field-tuned AFM quantum critical point at Hc~50T has been reported. We present new experimental evidence for a nematic character of this high-field phase. Electronic nematics are characterized by a lowered symmetry of the electronic system compared to the underlying lattice, in analogy to the directional alignment without translational order in nematic liquid crystals. Such phases appear in the copper- and iron-based high-temperature superconductors, and their role in establishing superconductivity remains an open question. In the nematic phase of CeRhIn5, a large in-plane resistivity anisotropy appears in the presence of a small in-plane field component. The anisotropy has little apparent connection to the lattice, rendering it a candidate for XY-nematicity. No anomalies are observed in the magnetic torque, suggesting the absence of metamagnetism. The appearance of nematic behavior in a prototypical heavy fermion superconductor highlights the interrelation of nematicity and unconventional superconductivity, suggesting nematicity to be common among correlated materials.

Presenters

  • Philip Moll

    Max Planck Institute for Chemical Physics of Solids, Max Planck Inst

Authors

  • Filip Ronning

    MPA-CMMS, Los Alamos National Laboratory, Los Alamos Natl Lab, Los Alamos National Laboratory, Condensed Matter and Magnetic Science Group, Los Alamos National Laboratory, Condensed Matter and Magnet Science Group, Los Alamos National Laboratory

  • Toni Helm

    Max Planck Institute for Chemical Physics of Solids, Max Planck Institute Dresden, MQM, Max Planck Inst CPFS

  • Kent Shirer

    Max Planck Institute for Chemical Physics of Solids, MQM, Max Planck Inst CPFS

  • Maja Bachmann

    Max Planck Institute for Chemical Physics of Solids

  • Luis Balicas

    Natl High Magnetic Field Lab, Nat. High Magn. Field Lab., Florida State University, FSU-NHMFL, National High Magnetic Field Lab, National High Magnetic Field Laboratory, Natl. High Magnetic Field Lab, Florida State University, High Field Magnet Lab, 1800 E. Paul Dirac Drive, National High Magnetic Field Laboratory, Natl High Magnetic Field Lab

  • Mun Chan

    National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos National Laboratory, National High Magnetic Field Laboratory

  • Brad Ramshaw

    Cornell University, Los Alamos National Labs, National High Magnetic Field Laboratory, Department of Physics, Cornell University, Laboratory of Atomic and Solid State Physics, Cornell University, Los Alamos National Laboratory, Laboratory for Atomic and Solid state Physics, Cornell University

  • Ross McDonald

    Los Alamos National Laboratory, National High Magnetic Field Laboratory, Pulsed Field Facility, Los Alamos National Lab, Los Alamos Natl Lab, LANL/NHMFL, NHMFL-PFF, Los Alamos National Laboratory, National High Magnetic Field Laboratory, LANL

  • Fedor Balakirev

    Los Alamos National Laboratory, Los Alamos National Lab NHMFL, National High Magnetic Field Laboratory, NHMFL-LANL, MS E536, National High Magnetic Field Laboratory, LANL

  • Marcelo Jaime

    Los Alamos Natl Lab, National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos National Laboratory, National High Magnetic Field Laboratory, NHMFL, LANL

  • Eric Bauer

    MPA-CMMS, Los Alamos National Laboratory, Los Alamos National Laboratory, Los Alamos Natl Lab, Condensed Matter and Magnetic Science Group, Los Alamos National Laboratory, Los Alamos National Lab, Condensed Matter and Magnet Science Group, Los Alamos National Laboratory

  • Philip Moll

    Max Planck Institute for Chemical Physics of Solids, Max Planck Inst