Electronic structure, quasiparticle renormalizations, and magnetic correlations in the alternating single-layer bilayer nickelate La5Ni3O11

Abstract

Using DFT+DMFT we study the normal-state electronic structure and magnetic correlations of the recently discovered alternating single-layer bilayer Raddlesden-Popper nickelate La5Ni3O11 (1212-LNO). Our results exhibit qualitative differences for the structurally distinct single-layer and bilayer Ni ions, implying the importance of confinement and orbital-dependent correlations. The Ni eg electronic states originating from the bilayer Ni ions form strongly renormalized quasiparticle bands with a large enhancement factor m*/m 3.5 and 4.2 for the Ni x2-y2 and 3z2-r2 orbitals, respectively. Moreover, the eg states of the single-layer Ni ions exhibit an orbital-selective Mott insulating state, with a narrow energy gap for the Ni 3z2-r2 states and metallic, strongly incoherent (non-Fermi-liquid) Ni x2-y2 ones. Our analysis of magnetic correlations suggests the formation of intertwined spin and charge density wave stripes in the bilayer NiO6 slab, in close similarity to the double-layer material. We refine two major instabilities, a leading one is associated with a wave vector Q=(13,13) (``up-down-0" spin pattern), competing with the bicollinear (14,14) (``up-up-down-down") stripe state. The single-layer Ni 3d electrons exhibit instability towards the N\'eel-type magnetic state. Under pressure, 1212-LNO undergoes an orbital-selective Mott insulator-to-metal phase transition, associated with metallization of the single-layer Ni eg states. As a result, the single-layer Ni eg bands exhibit non-Fermi-liquid (bad metal) behavior with strongly incoherent spectral weights near EF. We note that correlation effects result in a reconstruction of magnetic correlations as compared to that obtained within DFT. In fact, we observe a crossover from single-layer to double-layer dominated magnetic correlations.

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