Motivated by the recently reported signatures of superconductivity in trilayer La₄Ni₃O₁₀ under pressure, we comprehensively study this system using ab initio and random-phase approximation techniques. Without electronic interactions, the Ni d_{3z²-r²} orbitals show a bonding-antibonding and nonbonding splitting behavior via the O pz orbitals inducing a "trimer" lattice in La₄Ni₃O₁₀, analogous to the dimers of La₃Ni₂O₇. The Fermi surface consists of three electron sheets with mixed eg orbitals, and a hole and an electron pocket made up of the d_{3z²-r²} orbital, suggesting a Ni two-orbital minimum model. In addition, we find that superconducting pairing is induced in the s±-wave channel due to partial nesting between the M=(π,π) centered pockets and portions of the Fermi surface centered at the Γ=(0,0) point. With changing electronic density n, the s± instability remains leading and its pairing strength shows a domelike behavior with a maximum around n=4.2 (∼6.7% electron doping). The superconducting instability disappears at the same electronic density as that in the new 1313 stacking La₃Ni₂O₇, correlated with the vanishing of the hole pocket that arises from the trilayer sublattice, suggesting that the high-Tc superconductivity of La₃Ni₂O₇ does not originate from a trilayer and monolayer structure. Furthermore, we confirm the experimentally proposed spin state in La₄Ni₃O₁₀ with an in-plane (π, π) order and antiferromagnetic coupling between the top and bottom Ni layers, and spin zero in the middle layer.
No takes yet. Share an insight, caveat, or question.
Zhang et al. (2024) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: