Grace Pan1,Dan Ferenc Segedin1,Harrison LaBollita2,Qi Song1,Emilian Nica2,Berit Goodge3,Andrew Pierce1,Spencer Doyle1,Steve Novakov4,Denisse Córdova Carrizales1,Alpha N'Diaye5,Padraic Shafer5,Hanjong Paik3,John Heron4,Jarad Mason1,Amir Yacoby1,Lena Kourkoutis3,Onur Erten2,Charles Brooks1,Antia Botana2,Julia Mundy1
Harvard University1,Arizona State University2,Cornell University3,University of Michigan–Ann Arbor4,Lawrence Berkeley National Laboratory5
Grace Pan1,Dan Ferenc Segedin1,Harrison LaBollita2,Qi Song1,Emilian Nica2,Berit Goodge3,Andrew Pierce1,Spencer Doyle1,Steve Novakov4,Denisse Córdova Carrizales1,Alpha N'Diaye5,Padraic Shafer5,Hanjong Paik3,John Heron4,Jarad Mason1,Amir Yacoby1,Lena Kourkoutis3,Onur Erten2,Charles Brooks1,Antia Botana2,Julia Mundy1
Harvard University1,Arizona State University2,Cornell University3,University of Michigan–Ann Arbor4,Lawrence Berkeley National Laboratory5
Since the discovery of high-temperature superconductivity in the copper oxide materials, there have been sustained efforts to both understand the origins of this phase and discover new cuprate-like superconductors. One prime materials candidate has been the rare-earth nickelates and indeed superconductivity was recently discovered in the doped compound Nd<sub>0.8</sub>Sr<sub>0.2</sub>NiO<sub>2</sub>. Undoped NdNiO<sub>2</sub> belongs to a series of layered square-planar nickelates with chemical formula Nd<sub>n+1</sub>Ni<sub>n</sub>O<sub>2n+2</sub> and is known as the ‘infinite-layer’ (n = ∞) nickelate. Here, we present the superconducting and electronic properties of molecular beam epitaxy-synthesized Nd<sub>6</sub>Ni<sub>5</sub>O<sub>12</sub>, the quintuple-layer (n = 5) member of this series, which achieves optimal cuprate-like electron filling (3<i>d</i><sup>8.8</sup>) without chemical doping. We observe a superconducting transition beginning at ~13 K. [1] Electronic structure calculations, in tandem with magnetoresistive and spectroscopic measurements, suggest that Nd<sub>6</sub>Ni<sub>5</sub>O<sub>12</sub> interpolates between cuprate-like and infinite-layer nickelate-like behavior. By engineering a distinct superconducting nickelate, we identify the square-planar nickelates as a new family of superconductors which can be tuned via both doping and dimensionality. In part II of this talk, we further expound on the synthetic strategies of the layered nickelates including Nd<sub>6</sub>Ni<sub>5</sub>O<sub>12</sub>.<br/>[1] GA Pan et al. Superconductivity in a quintuple-layer square-planar nickelate. arXiv:2109.09726.<br/>[2] D Ferenc Segedin et al. Superconducting Quintuple-layer Square-planar Nickelates: Synthetic Strategies and Challenges (Part II). MRS Bulletin Spring 2022.