Electronic structure, magnetic properties, and pairing tendencies of the copper-based honeycomb lattice Na2Cu2TeO6

Ling-Fang Lin, Rahul Soni, Yang Zhang, Shang Gao, Adriana Moreo, Gonzalo Alvarez, Andrew D. Christianson, Matthew B. Stone, and Elbio Dagotto
Phys. Rev. B 105, 245113 – Published 10 June 2022

Abstract

Spin-1/2 chains with alternating antiferromagnetic (AFM) and ferromagnetic (FM) couplings have attracted considerable interest due to the topological character of their spin excitations. Here, using density functional theory and density-matrix renormalization-group (DMRG) methods, we have systematically studied the dimerized chain system Na2Cu2TeO6 with a d9 electronic configuration. Near the Fermi level, in the nonmagnetic phase the dominant states are mainly contributed by the Cu 3dx2y2 orbitals highly hybridized with the O 2p orbitals, leading to an “effective” single-orbital low-energy model. By calculating the relevant hoping amplitudes, we explain the size and sign of the exchange interactions in Na2Cu2TeO6. In addition, a single-orbital Hubbard model is constructed for this dimerized chain system where the quantum fluctuations are taken into account. Both AFM and FM couplings (leading to an state) along the chain were found in our DMRG and Lanczos calculations, in agreement with density functional theory and neutron-scattering results. The hole pairing binding energy ΔE is predicted to be negative at Hubbard U11eV, suggesting incipient pairing tendencies.

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  • Received 27 March 2022
  • Revised 17 May 2022
  • Accepted 31 May 2022

DOI:https://doi.org/10.1103/PhysRevB.105.245113

©2022 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Ling-Fang Lin1, Rahul Soni1,2, Yang Zhang1, Shang Gao2,3, Adriana Moreo1,2, Gonzalo Alvarez4, Andrew D. Christianson2, Matthew B. Stone3, and Elbio Dagotto1,2

  • 1Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
  • 2Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 4Computational Sciences & Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

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Issue

Vol. 105, Iss. 24 — 15 June 2022

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