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Second dome of superconductivity in YBa2Cu3O7 at high pressure

Johannes Nokelainen1,2,3,4,*, Matthew E. Matzelle1,2, Christopher Lane5, Nabil Atlam1,2, Ruiqi Zhang6, Robert S. Markiewicz1,2, Bernardo Barbiellini4,1,2, Jianwei Sun6, and Arun Bansil1,2,†

  • 1Department of Physics, Northeastern University, Boston, Massachusetts 02115, USA
  • 2Quantum Materials and Sensing Institute, Northeastern University, Burlington, Massachusetts 01803, USA
  • 3Department of Physics and Astrophysics, Howard University, Washington, DC 20059, USA
  • 4Department of Physics, School of Engineering Science, LUT University, FI-53850 Lappeenranta, Finland
  • 5Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 6Department of Physics and Engineering Physics, Tulane University, New Orleans, Louisiana 70118, USA

  • *Contact author: j.nokelainen@northeastern.edu
  • †Contact author: ar.bansil@northeastern.edu

Phys. Rev. B 110, L020502 – Published 11 July, 2024

DOI: https://doi.org/10.1103/PhysRevB.110.L020502

Abstract

Evidence is growing that a second dome of high-Tc superconductivity can be accessed in the cuprates by increasing the doping beyond the first dome. Here, we use ab initio methods without invoking any free parameters, such as the Hubbard U, to reveal that pressure could turn YBa2Cu3O7 into an ideal candidate for second dome superconductivity, displaying the predicted signature of strongly hybridized dx2−y2 and dz2 orbitals. Notably, pressure is found to induce a phase transition replacing the antiferromagnetic phases with an orbitally degenerate d−d phase. Our study suggests that the origin of the second dome is correlated with the oxygen-hole fraction in the CuO2 planes and the collapse of the pseudogap phase.

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