English

Infinite Layer LaNiO(2): Ni(1+)is not Cu(2+)

Strongly Correlated Electrons 2009-11-10 v1 Materials Science

Abstract

The Ni ion in LaNiO2_2 has the same formal ionic configuration 3d93d^9 as does Cu in isostructural CaCuO2_2, but it is reported to be nonmagnetic and probably metallic whereas CaCuO2_2 is a magnetic insulator. From ab initio calculations we trace its individualistic behavior to (1) reduced 3d2p3d-2p mixing due to an increase of the separation of site energies (ϵdϵp\epsilon_d - \epsilon_p) of at least 2 eV, and (2) important Ni 3d(3z2r2)3d(3z^2-r^2) mixing with La 5d(3z2r2)5d(3z^2-r^2) states that leads to Fermi surface pockets of La 5d5d character that hole-dope the Ni 3d band.Correlation effects do not appear to be large in LaNiO2_2. However, ad hoc increase of the intraatomic repulsion on the Ni site (using the LDA+U method) is found to lead to a novel correlated state: (i) the transition metal d(x2y2)d(x^2-y^2) and d(3z2r2)d(3z^2-r^2) states undergo consecutive Mott transitions, (ii) their moments are antialigned leading (ideally) to a "singlet" ion in which there are two polarized orbitals, and (iii) mixing of the upper Hubbard 3d(3z2r2)3d(3z^2-r^2) band with the La 5d(xy)5d(xy) states leaves considerable transition metal 3d character in a band pinned to the Fermi level. The magnetic configuration is more indicative of a Ni2+^{2+} ion in this limit, although the actual charge changes little with U.

Keywords

Cite

@article{arxiv.cond-mat/0405570,
  title  = {Infinite Layer LaNiO(2): Ni(1+)is not Cu(2+)},
  author = {K. -W. Lee and W. E. Pickett},
  journal= {arXiv preprint arXiv:cond-mat/0405570},
  year   = {2009}
}

Comments

7 pages, 8 figures

R2 v1 2026-07-22T11:03:36.777Z