Following the successful prediction of the superconducting phase diagram for infinite-layer nickelates, here we calculate the superconducting Tc vs. the number of layers n for finite-layer nickelates using the dynamical vertex approximation. To this end, we start with density functional theory, and include local correlations non-perturbatively by dynamical mean-field theory for n = 2–7. For all n, the Ni dx2−y2 orbital crosses the Fermi level, but for n > 4 there are additional (π, π) pockets or tubes that slightly enhance the layer-averaged hole doping of the dx2−y2 orbitals beyond the leading 1/n contribution stemming from the valence electron count. We finally calculate Tc for the single-orbital dx2−y2 Hubbard model by dynamical vertex approximation.
Superconducting phase diagram of finite-layer nickelates Ndn+1NinO2n+2 / Hausoel, A., Di Cataldo, S., Kitatani, M., Janson, O., Held, K.. - In: NPJ QUANTUM MATERIALS. - ISSN 2397-4648. - 10:1(2025), pp. 1-6. [10.1038/s41535-025-00786-z]
Superconducting phase diagram of finite-layer nickelates Ndn+1NinO2n+2
Di Cataldo S.Secondo
Investigation
;
2025
Abstract
Following the successful prediction of the superconducting phase diagram for infinite-layer nickelates, here we calculate the superconducting Tc vs. the number of layers n for finite-layer nickelates using the dynamical vertex approximation. To this end, we start with density functional theory, and include local correlations non-perturbatively by dynamical mean-field theory for n = 2–7. For all n, the Ni dx2−y2 orbital crosses the Fermi level, but for n > 4 there are additional (π, π) pockets or tubes that slightly enhance the layer-averaged hole doping of the dx2−y2 orbitals beyond the leading 1/n contribution stemming from the valence electron count. We finally calculate Tc for the single-orbital dx2−y2 Hubbard model by dynamical vertex approximation.| File | Dimensione | Formato | |
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Hausoel_Superconducting-phase-diagram_2025.pdf
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