Characterization of two electronic subsystems in cuprates through optical conductivity

C. M. N. Kumar, A. Akrap, C. C. Homes, E. Martino, B. Klebel-Knobloch, W. Tabis, O. S. Barišić, D. K. Sunko, and N. Barišić
Phys. Rev. B 107, 144515 – Published 27 April 2023

Abstract

Understanding the physical properties of unconventional superconductors as well as of other correlated materials presents a formidable challenge. Their unusual evolution with doping, frequency, and temperature has frequently led to non-Fermi-liquid (non-FL) interpretations. Optical conductivity is a major challenge in this context. Here, the optical spectra of two archetypal cuprates, underdoped HgBa2CuO4+δ and optimally doped Bi2Sr2CaCu2O8+δ, are interpreted based on the standard Fermi-liquid (FL) paradigm. At both dopings, perfect frequency-temperature FL scaling is found to be modified by the presence of a second, gapped electronic subsystem. This non-FL component emerges as a well-defined mid-infrared spectral feature after the FL contribution, determined independently by transport, is subtracted. Temperature, frequency, and doping evolution of the MIR feature identify a gapped rather than dissipative response. In contrast, the dissipative response is found to be relevant for pnictides and ruthenates. Such an unbiased FL/non-FL separation is extended across the cuprate phase diagram, capturing all the key features of the normal state and providing a natural explanation why the superfluid density is attenuated on the overdoped side. Thus, we obtain a unified interpretation of optical responses and transport measurements in all analyzed physical regimes and all analyzed compounds.

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  • Received 1 July 2022
  • Revised 7 April 2023
  • Accepted 12 April 2023

DOI:https://doi.org/10.1103/PhysRevB.107.144515

©2023 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

C. M. N. Kumar1,2,3, A. Akrap4, C. C. Homes5,6, E. Martino7, B. Klebel-Knobloch1, W. Tabis1,8, O. S. Barišić2, D. K. Sunko9, and N. Barišić1,9,*

  • 1Institute of Solid State Physics, TU Wien, 1040 Vienna, Austria
  • 2Institute of Physics, Bijenička cesta 46, HR-10000 Zagreb, Croatia
  • 3The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, 152 Radzikowskiego Strasse, 31-342 Krakow, Poland
  • 4Department of Physics, University of Fribourg, Chemin du Musée 3, CH-1700 Fribourg, Switzerland
  • 5Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA
  • 6National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, USA
  • 7Institute of Physics, École Polytechnique Fédéral de Lausanne (EPFL), CH-1015 Lausanne, Switzerland
  • 8AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, 30-059 Krakow, Poland
  • 9Department of Physics, Faculty of Science, University of Zagreb, Bijenička cesta 32, HR-10000 Zagreb, Croatia

  • *nbarisic@phy.hr

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Issue

Vol. 107, Iss. 14 — 1 April 2023

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