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Observation of Three-Dimensional Flat Bands and Dirac Cones in a Pyrochlore Superconductor

ORAL

Abstract

Emergent phases often appear when the electronic kinetic energy is comparable to the Coulomb interactions. One approach to seek material systems as hosts of such emergent phases is to realize localization of electronic wavefunctions due to the geometric frustration inherent in the crystal structure, resulting in flat electronic bands. Recently, such efforts have found a wide range of exotic phases in the two-dimensional kagome lattice, including magnetic order, time-reversal symmetry breaking charge order, nematicity, and superconductivity. However, the interlayer coupling of the kagome layers disrupts the destructive interference needed to completely quench the kinetic energy. Here we experimentally demonstrate that an interwoven kagome network—a pyrochlore lattice—can host a three-dimensional localization of electron wavefunctions. In particular, through a combination of angle-resolved photoemission spectroscopy, fundamental lattice model and density functional theory calculations, we present the novel electronic structure of a pyrochlore superconductor, CeRu2. We find striking flat bands along all momentum directions. We further find three-dimensional gapless Dirac cones predicted originally by theory in the diamond lattice space group with nonsymmorphic symmetry. Our work establishes the pyrochlore structure as a promising lattice platform to realize and tune novel emergent phases intertwining topology and many-body interactions.

Presenters

  • Jianwei Huang

    Rice University

Authors

  • Jianwei Huang

    Rice University

  • Chandan Setty

    Rice University

  • Liangzi Deng

    University of Houston, Department of Physics and Texas Center for Superconductivity, University of Houston

  • Jingyang You

    National University of Singapore

  • Hongxiong Liu

    Institute of Physics, Chinese Academy of Sciences, Institute of Physics, Chinese Academy of Sciences, Beijing, China, Chinese Academy of Sciences

  • Sen Shao

    Nanyang Technological University

  • Ji Seop Oh

    University of California Berkeley

  • Yucheng Guo

    Rice University

  • Yichen Zhang

    Rice University

  • Ziqin Yue

    Rice University

  • Jia-Xin Yin

    2Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, New Jersey 08544, USA, Princeton University

  • Makoto Hashimoto

    SLAC - Natl Accelerator Lab

  • Donghui Lu

    SLAC - Natl Accelerator Lab

  • Sergey Gorovikov

    Canadian Light Source, Canadian Lightsource

  • Pengcheng Dai

    Rice University

  • M. Zahid M Hasan

    Princeton University

  • Yuan P Feng

    National University of Singapore, Natl Univ of Singapore

  • Robert J Birgeneau

    University of California, Berkeley

  • Youguo Shi

    Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Institute of Physics, Chinese Academy of Sciences, Beijing, China, Chinese Academy of Sciences

  • Ching-Wu W Chu

    University of Houston, Department of Physics and Texas Center for Superconductivity, University of Houston

  • Guoqing Chang

    Nanyang Technological University, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, 637371 Singapore

  • Qimiao Si

    Rice University

  • Ming Yi

    Rice University