Universal flow of charge and heat near quantum criticality in ultraclean graphene

ORAL

Abstract

Over the past decade, electron fluids in graphene have garnered significant attention because of their unique electrical and magnetic properties. Near the charge neutrality point, graphene is expected to behave like a “Dirac fluid” - a fluid of massless Dirac fermions described by a universal electrical conductivity σQ. Despite several experimental reports on the fluid-like electronic transport in graphene, there has been no direct experimental evidence of σQ. In this work, we have fabricated hBN-encapsulated ultraclean graphene devices with high electron mobilities (~100 m2 V-1 s-1) and performed electrical and thermal transport from room temperature down to 20 K. We observe that the quantum critical conductivity of our devices approaches the universal bound of (4±1) e2/h near room temperature. Additionally, we report a giant violation of the Wiedemann-Franz Law near the charge neutrality point across a range of temperatures and find the η/s ratio for our devices, from independent measurements of shear viscosity and entropy density, to be within a factor of four of the holographic bound. Our experimental observations are also quantitatively consistent with that of a non-Galilean-invariant Dirac fluid.

*A.G. acknowledges support from a project under DST NanoMission and J. C. Bose Fellowship. P.P. and A.G. thank MoE, GoI for the Prime Minister's Research Fellowship. K.W. and T.T. acknowledge support from JSPS KAKENHI (Grant Numbers 19H05790 and 21H05233).

Publication: Universality in quantum critical flow of charge and heat in ultra-clean graphene, A. Majumdar, et al., (Manuscript under preparation)

Presenters

  • Aniket Majumdar

    • Indian Institute of Science

Authors

  • Aniket Majumdar

    • Indian Institute of Science
  • Nisarg Chadha

    • Harvard University
  • Pritam Pal

    • Indian Institute of Science
  • Akash Gugnani

    • Indian Institute of Science
  • Bhaskar Ghawri

    • Indian Institute of Science
  • Kenji Watanabe

    • National Institute for Materials Science
    • NIMS
    • Research Center for Functional Materials, National Institute for Materials Science
    • Research Center for Electronic and Optical Materials, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Japan
    • Research Center for Functional Materials, National Institute of Material Science, Tsukuba, Japan
    • National Institute of Materials Science
    • Advanced Materials Laboratory, National Institute for Materials Science
  • Takashi Taniguchi

    • National Institute for Materials Science
    • International Center for Materials Nanoarchitectonics, National Institute for Materials Science
    • Research Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Japan
    • International Center for Materials Nanoarchitectonics, National Institute of Material Science, Tsukuba, Japan
    • Advanced Materials Laboratory, National Institute for Materials Science
  • Subroto Mukerjee

    • Indian Institute of Science Bangalore
  • Arindam Ghosh

    • Indian Institute of Science