Superconductivity in an infinite-layer nickelate

The discovery of unconventional superconductivity in (La,Ba)2CuO4 (ref. 1) has motivated the study of compounds with similar crystal and electronic structure, with the aim of finding additional superconductors and understanding the origins of copper oxide superconductivity. Isostructural examples include bulk superconducting Sr2RuO4 (ref. 2) and surface-electron-doped Sr2IrO4, which exhibits spectroscopic signatures consistent with a superconducting gap3,4, although a zero-resistance state has not yet been observed. This approach has also led to the theoretical investigation of nickelates5,6, as well as thin-film heterostructures designed to host superconductivity. One such structure is the LaAlO3/LaNiO3 superlattice7–9, which has been recently proposed for the creation of an artificially layered nickelate heterostructure with a singly occupied $${d}_{{x}^{2}-{y}^{2}}$$ dx2-y2 band. The absence of superconductivity observed in previous related experiments has been attributed, at least in part, to incomplete polarization of the e g orbitals10. Here we report the observation of superconductivity in an infinite-layer nickelate that is isostructural to infinite-layer copper oxides11–13. Using soft-chemistry topotactic reduction14–20, NdNiO2 and Nd0.8Sr0.2NiO2 single-crystal thin films are synthesized by reducing the perovskite precursor phase. Whereas NdNiO2 exhibits a resistive upturn at low temperature, measurements of the resistivity, critical current density and magnetic-field response of Nd0.8Sr0.2NiO2 indicate a superconducting transition temperature of about 9 to 15 kelvin. Because this compound is a member of a series of reduced layered nickelate crystal structures21–23, these results suggest the possibility of a family of nickelate superconductors analogous to copper oxides24 and pnictides25. Superconductivity is demonstrated in an infinite-layer nickelate similar to infinite-layer copper oxides, which is synthesized using soft- chemistry topotactic reduction of the perovskite precursor phase.

[1]  Nazzal,et al.  Systematic study of insulator-metal transitions in perovskites RNiO3 (R=Pr,Nd,Sm,Eu) due to closing of charge-transfer gap. , 1992, Physical review. B, Condensed matter.

[2]  I. Božović,et al.  High-precision measurement of magnetic penetration depth in superconducting films. , 2016, The Review of scientific instruments.

[3]  V. Poltavets,et al.  La3Ni2O6: a new double T'-type nickelate with infinite Ni1+/2+O2 layers. , 2006, Journal of the American Chemical Society.

[4]  K. Müller,et al.  Possible highTc superconductivity in the Ba−La−Cu−O system , 1986 .

[5]  K. Lee,et al.  Infinite-layer LaNiO 2 : Ni 1 + is , 2022 .

[6]  A. Chikamatsu,et al.  Formation of defect-fluorite structured NdNiOxHy epitaxial thin films via a soft chemical route from NdNiO3 precursors. , 2016, Dalton transactions.

[7]  M. Mizumaki,et al.  Orientation Change of an Infinite-Layer Structure LaNiO2 Epitaxial Thin Film by Annealing with CaH2 , 2010 .

[8]  J. Mitchell,et al.  Large orbital polarization in a metallic square-planar nickelate , 2017, Nature Physics.

[9]  M. Hayward,et al.  Sodium Hydride as a Powerful Reducing Agent for Topotactic Oxide Deintercalation: Synthesis and Characterization of the Nickel(I) Oxide LaNiO2 , 1999 .

[10]  Iron-based superconductors: Current status of materials and pairing mechanism , 2015, 1504.04919.

[11]  F. Lichtenberg,et al.  Superconductivity in a layered perovskite without copper , 1994, Nature.

[12]  Signature of high temperature superconductivity in electron doped Sr2IrO4 , 2015, 1506.06557.

[13]  P. Lacorre Passage from T-type to T′-type arrangement by reducing R4Ni3O10 to R4Ni3O8 (R = La, Pr, Nd) , 1992 .

[14]  A. Malashevich,et al.  Orbital engineering in symmetry-breaking polar heterostructures. , 2015, Physical review letters.

[15]  M. Hayward,et al.  Synthesis of the infinite layer Ni(I) phase NdNiO2+x by low temperature reduction of NdNiO3 with sodium hydride , 2003 .

[16]  M. R. Norman,et al.  From quantum matter to high-temperature superconductivity in copper oxides , 2015, Nature.

[17]  Xin Wang,et al.  Dynamical mean-field theory of nickelate superlattices. , 2011, Physical review letters.

[18]  Zhang,et al.  Effective Hamiltonian for the superconducting Cu oxides. , 1988, Physical review. B, Condensed matter.

[19]  P. Levitz,et al.  Reduced forms of LaNiO3 perovskite. Part 1.—Evidence for new phases: La2Ni2O5 and LaNiO2 , 1983 .

[20]  M. Mizumaki,et al.  Reversible changes of epitaxial thin films from perovskite LaNiO3 to infinite-layer structure LaNiO2 , 2009 .

[21]  B. J. Kim,et al.  Observation of a d-wave gap in electron-doped Sr2IrO4 , 2015, Nature Physics.

[22]  Hideki Yamamoto,et al.  Direct observation of infinite NiO2 planes in LaNiO2 films , 2016 .

[23]  M. Azuma,et al.  Superconductivity at 110 K in the infinite-layer compound (Sr1-xCax)1-yCuO2 , 1992, Nature.

[24]  A. Manthiram,et al.  Electron-doped superconductivity at 40 K in the infinite-layer compound Sr1–yNdyCu02 , 1991, Nature.

[25]  K. Lee,et al.  Infinite-layerLaNiO2: Ni1+is notCu2+ , 2004, cond-mat/0405570.

[26]  Alonso,et al.  Influence of carrier injection on the metal-insulator transition in electron- and hole-doped R1-xAxNiO3 perovskites. , 1995, Physical review. B, Condensed matter.

[27]  A. S. Cooper,et al.  Electron-hole doping of the metal-insulator transition compound RENiO3 , 1994 .

[28]  K. Held,et al.  Turning a nickelate Fermi surface into a cupratelike one through heterostructuring. , 2008, Physical review letters.

[29]  D. Muller,et al.  Why some interfaces cannot be sharp , 2005, cond-mat/0510491.

[30]  K. Lee,et al.  Infinite-layer LaNiO2: Ni1+ is not Cu2+ , 2004 .

[31]  D. Murphy,et al.  The parent structure of the layered high-temperature superconductors , 1988, Nature.

[32]  J. Chaloupka,et al.  Orbital order and possible superconductivity in LaNiO3/LaMO3 superlattices. , 2008, Physical review letters.

[33]  V. Anisimov,et al.  Electronic structure of possible nickelate analogs to the cuprates , 1999 .