General trends of electronic structures, superconducting pairing, and magnetic correlations in the Ruddlesden-Popper nickelate m-layered superconductors Lam+1NimO3m+1

Abstract

We report a comprehensive theoretical analysis of the Ruddlesden-Popper layered nickelates Lam+1NimO3m+1 (m = 1 to 6) under pressure. Our results suggest that, while these Ruddlesden-Popper layered nickelates display many similarities, they also show noticeable differences. The Ni d3z2-r2 orbitals display bonding-antibonding, or bonding-antibonding-nonbonding, characteristic splittings, depending on the even or odd number of stacking layers m. In addition, the ratio of the in-plane interorbital hopping between d3z2-r2 and dx2-y2 orbitals and in-plane intraorbital hopping between dx2-y2 orbitals was found to be large in Lam+1NimO3m+1 (m = 1 to 6), and this ratio increases from m = 1 to m = 6, suggesting that the in-plane hybridization will increase as the layer number m increases. In contrast to the dominant s--wave state driven by spin fluctuations in the bilayer La3Ni2O7 and trilayer La4Ni3O10, two nearly degenerate dx2-y2-wave and s-wave leading states were obtained in the four-layer stacking La5Ni4O13 and five-layer stacking La6Ni5O16. The leading s-wave state was recovered in the six-layer material La7Ni6O19. In general, at the level of the random phase approximation treatment, the superconducting transition temperature Tc decreases in stoichiometric bulk systems from the bilayer La3Ni2O7 to the six-layer La7Ni6O19, despite the m dependent dominant pairing. Both in-plane and out-of-plane magnetic correlations are found to be quite complex. Within the in-plane direction, we obtained the peak of the magnetic susceptibility at q = (0.6 π, 0.6 π) for La5Ni4O13 and La7Ni6O19, and at q = (0.7 π, 0.7 π) for La6Ni5O16.

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