Electronic structures and topological properties in nickelates Ln(n+1)Ni(n)O(2n+2)

After the significant discovery of the hole-doped nickelate compound Nd(0.8)Sr(0.2)NiO(2), analyses of the electronic structure, orbital components, Fermi surfaces and band topology could be helpful to understand the mechanism of its superconductivity. Based on first-principle calculations, we find that Ni [Formula: see text] states contribute the largest Fermi surface. The [Formula: see text] states form an electron pocket at Γ, while 5d(xy) states form a relatively bigger electron pocket at A. These Fermi surfaces and symmetry characteristics can be reproduced by our two-band model, which consists of two elementary band representations: B(1g)@1a ⊕ A(1g)@1b. We find that there is a band inversion near A, giving rise to a pair of Dirac points along M-A below the Fermi level upon including spin-orbit coupling. Furthermore, we perform density functional theory based Gutzwiller (DFT+Gutzwiller) calculations to treat the strong correlation effect of Ni 3d orbitals. In particular, the bandwidth of [Formula: see text] has been renormalized largely. After the renormalization of the correlated bands, the Ni 3d(xy) states and the Dirac points become very close to the Fermi level. Thus, a hole pocket at A could be introduced by hole doping, which may be related to the observed sign change of the Hall coefficient. By introducing an additional Ni 3d(xy) orbital, the hole-pocket band and the band inversion can be captured in our modified model. Besides, the nontrivial band topology in the ferromagnetic two-layer compound La(3)Ni(2)O(6) is discussed and the band inversion is associated with Ni [Formula: see text] and La 5d(xy) orbitals.