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Optical properties of severely overdoped La<sub>1.75</sub>Sr<sub>0.25</sub>CuO<sub>4</sub>

ORAL

Abstract

The temperature dependence of the optical properties of the severely overdoped cuprate La1.75Sr0.25CuO4 have been determined above and below the critical temperature Tc ~16 K over a wide frequency range for light polarized in the a-b plane. The real part of the optical conductivity can be reproduced reasonably well at low frequency using a simple Drude model, yielding an estimate for the plasma frequency wpD ~ 9300 cm-1. Below Tc the superconducting plasma frequency wps ~ 2700 cm-1 is determined from the Ferrell-Glover-Tinkham sum rule, indicating that less than 8% of the free carriers collapse into the superconducting condensate, in agreement with a recent study [1]. However, there is unusual structure below ~0.1 eV that suggests that the free-carrier scattering rate is strongly renormalized with frequency. In addition, the nature of the magnetic susceptibility through the superconducting transition suggests that this compound may not be homogeneous.

[1] I. Bozovic et al., Nature 536, 309 (2016).

Presenters

  • Christopher Homes

    Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory

Authors

  • Christopher Homes

    Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory

  • Genda Gu

    Brookhaven National Laboratory, Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory, Brookhaven national lab, Condensed Matter Physics and Materials Science, Brookhaven National Laboratory, Brookhaven National Lab, Condensed Matter Physics and Material Science, Brookhaven National Laboratory, Upton, NY, United States, Brookhaven National Laboratories, Condensed Matter Physics and Material Science Division, Brookhaven National Laboratory

  • P. M. Lozano

    Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory

  • Qiang Li

    Brookhaven National Laboratory, Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory, Condensed Matter Physics and Material Science Division, Brookhaven National Laboratory