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Electronic correlations in the ultranarrow energy band compound Pb9Cu(PO4)6O: A DFT+DMFT study

Dmitry M. Korotin1,2,*, Dmitry Y. Novoselov1,2,3, Alexey O. Shorikov1,2,3, Vladimir I. Anisimov1,2,3, and Artem R. Oganov2,4

  • 1M. N. Mikheev Institute of Metal Physics of the Ural Branch of the Russian Academy of Sciences, 18 S. Kovalevskaya Street, Yekaterinburg 620108, Russia
  • 2Skolkovo Institute of Science and Technology, 30 Bolshoy Boulevard, Building 1, Moscow 121205, Russia
  • 3Department of Theoretical Physics and Applied Mathematics, Ural Federal University, 19 Mira Street, Yekaterinburg 620002, Russia
  • 4Moscow Institute of Physics and Technology, 9 Institutskiy Lane, Dolgoprudny, Moscow Region 141701, Russia

  • *dmitry@korotin.name

Phys. Rev. B 108, L241111 – Published 15 December, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L241111

Abstract

We present results of investigations on the correlated nature of electronic states crossing the Fermi level in Pb9Cu(PO4)6O (also referred to as LK-99) obtained within the DFT+DMFT approach. We found that the band structure in the vicinity of the Fermi level is formed by extremely narrow Cud states and p states of extra O weakly hybridized with each other. Coulomb correlations between Cud electrons open the band gap between Cu dxz/dyz and the extra-O p states that form the top of the valence band. Our conclusion is that the extra-oxygen p states play a significant role in the electronic properties and LK-99 cannot be mapped onto a two-band Hubbard model. We also conclude that doping with electrons will turn the stoichiometric Pb9Cu(PO4)6O into a metal, whereas the result of doping with holes is less certain.

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