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Layered Metals as Polarized Transparent Conductors

ORAL

Abstract

The quest to improve transparent conductors balances two key goals: increasing electrical conductivity and increasing optical transparency. To improve both simultaneously is hindered by the physical limitation that good metals with high electrical conductivity have large carrier densities that push the plasma edge into the ultra-violet range. Transparent conductors are compromises between electrical conductivity, requiring mobile electrons, and optical transparency based on immobile charges to avoid screening of visible light. Technological solutions reflect this trade-off, achieving the desired transparencies by reducing the conductor thickness or carrier density at the expense of a lower conductance. Here we demonstrate that highly anisotropic crystalline conductors offer an alternative solution, avoiding this compromise by separating the directions of conduction and transmission. Materials with a quasi-two-dimensional electronic structure have a plasma edge well below the range of visible light while maintaining excellent in-plane conductivity. We demonstrate that slabs of the layered oxides Sr2RuO4 and Tl2Ba2CuO6+d are optically transparent even at macroscopic thicknesses >2mm for c-axis polarized light. Underlying this observation is the fabrication of out-of-plane slabs by focused ion beam milling. This work provides a glimpse into future technologies, such as highly polarized and addressable optical screens, that advancements in a-axis thin film growth will enable.

Presenters

  • Carsten Putzke

    Max Planck Institute of the Structure & Dynamics of Matter, Max Planck Institute for the Structure and Dynamics of Matter

Authors

  • Carsten Putzke

    Max Planck Institute of the Structure & Dynamics of Matter, Max Planck Institute for the Structure and Dynamics of Matter

  • Chunyu Guo

    Max Planck Institute for the Structure and Dynamics of Matte, Ecole Polytechnique Federale de Lausanne

  • Vincent M Plisson

    Boston College

  • Martin Kroner

    ETH Zurich

  • Thibault Chervy

    NTT Research Inc

  • Matteao Simoni

    ETH Zurich

  • Pim Wevers

    ETH Zurich

  • Maja D Bachmann

    Stanford Univ

  • John R Cooper

    Cavendish Laboratory Cambridge

  • Antony Carrington

    University of Bristol

  • Naoki Kikugawa

    National Institute for Material Science

  • Jennifer Fowlie

    Stanford University, Stanford University, SLAC National Accelerator Laboratory

  • Stefano Gariglio

    Univ of Geneva

  • Andrew Mackenzie

    Max Planck Institute for Chemical Physics of Solids, Max-Planck-Institute for the Chemical Physics of Solids, Max-Planck-Institute for Chemical Physics of Solids

  • Kenneth S Burch

    Boston College

  • Atac Imamoglu

    ETH Zurich

  • Philip J Moll

    Max Planck Institute for the Structure & Dynamics of Matter