Abstract

The discovery of superconductivity in infinite-layer nickelates has added a new family of materials to the fascinating growing class of unconventional superconductors. By incorporating the strongly correlated multi-orbital nature of the low-energy electronic degrees of freedom, we compute the leading superconducting instability from magnetic fluctuations relevant for infinite-layer nickelates. Specifically, by properly including the doping dependence of the Ni dx2−y2d_{x^2-y^2} and dz2d_{z^2} orbitals as well as the self-doping band, we uncover a transition from dd-wave pairing symmetry to nodal s±s_\pm superconductivity, driven by strong fluctuations in the dz2d_{z^2}-dominated orbital states. We discuss the properties of the resulting superconducting condensates in light of recent tunneling and penetration depth experiments probing the detailed superconducting gap structure of these materials.

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