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Paramagnons and high-temperature superconductivity in mercury-based cuprates

ORAL

Abstract

High-temperature superconductivity in the cuprates is realized upon doping antiferromagnetic parent compounds, in which spin excitations have a bandwidth of a few hundred meV. At such high energies, paramagnons and two-magnon excitations are known to persist well into and beyond the superconducting doping range [1,2,3], but it remains unclear to what extent they contribute to Cooper pairing [4] or how the magnetic and superconducting energy scales are related to each other. We have used resonant inelastic photon (Raman, X-ray) scattering to study the first two members of the Hg-family of cuprates, HgBa2CuO4+d and HgBa2CaCu2O6+d, which have nearly identical crystal structure in the charge-reservoir layers but different electronic environment in the quintessential Cu-O layers. We find that the latter compound, which has higher Tc and larger superconducting gap, also has considerably higher magnetic excitation energies.
[1] Nat. Phys. 7, 725 (2011).
[2] Nat. Mater. 12, 1019 (2013).
[3] Phys. Rev. Lett. 111, 187001 (2013).
[4] Phys. Rev. Lett. 108, 227003 (2012).

Presenters

  • Guanhong He

    International Cent re for Quantum Materials, School of Physics, Peking University, Beijing, Peking Univ

Authors

  • Lichen Wang

    International Cent re for Quantum Materials, School of Physics, Peking University, Beijing, Peking Univ

  • Guanhong He

    International Cent re for Quantum Materials, School of Physics, Peking University, Beijing, Peking Univ

  • Zichen Yang

    Solid State spectroscopy, Max Planck Institute for Solid State Research

  • Mirian Garcia-Fernnandez

    Diamond Light Source, Diamond Light Source, UK, Diamond Light Source, Harwell Science & Innovation Campus

  • Abhishek Nag

    Diamond Light Source, Diamond Light Source, Harwell Science & Innovation Campus

  • Ke-jin Zhou

    Diamond Light Source, Diamond Light Source, UK, Diamond Light Source, Harwell Science & Innovation Campus

  • Matteo Minola

    Max-Planck-Institute for Solid State Research, Heisenbergstrasse 1, 70569 Stuttgart, Germany, Solid State spectroscopy, Max Planck Institute for Solid State Research

  • Matthieu Le Tacon

    Institute for Quantum Materials and Technologies, Karlsruhe Institute of Technology, Institute for Quantum Materials and Technologies, Karlsruhe Institute of Technology, Germany

  • Bernhard Keimer

    Max Planck Inst for Solid State Research, Max-Planck-Institute for Solid State Research, Heisenbergstrasse 1, 70569 Stuttgart, Germany, Max Planck Institute for Solid State Physics, Max Planck Institute for Solid State Research, Solid State spectroscopy, Max Planck Institute for Solid State Research, Max Planck Institute for Solid State Research, Stuttgart, Germany

  • Yingying Peng

    International Cent re for Quantum Materials, School of Physics, Peking University, Beijing, Peking Univ

  • Yuan Li

    International Center for Quantum Materials, School of Physics, Peking University, Peking University, Peking Univ, International Cent re for Quantum Materials, School of Physics, Peking University, Beijing, Peking Univ