4.8 Article

Nickelate Superconductivity without Rare-Earth Magnetism: (La,Sr)NiO2

Journal

ADVANCED MATERIALS
Volume 33, Issue 45, Pages -

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/adma.202104083

Keywords

nickelates; rare-earth; superconductivity; thin films

Funding

  1. US Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering [DE-AC02-76SF00515]
  2. Gordon and Betty Moore Foundation's Emergent Phenomena in Quantum Systems Initiative [GBMF9072]
  3. Department of Defense Air Force Office of Scientific Research [FA 9550-16-1-0305]
  4. NSF MRSEC Program [DMR-1719875]
  5. Cornell University
  6. Weill Institute
  7. Kavli Institute at Cornell
  8. National Science Foundation [DMR-1719875, DMR-1539918]
  9. [NSF-MRI-1429155]

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Through material optimization, a significant portion of the La1-xSrxNiO2 phase diagram can enter the realm of superconductivity, with a maximum onset temperature of approximately 9 K at x = 0.20. An unexpected indication of a superconducting ground state was also observed in undoped LaNiO2. Combining the results of different rare-earth elements in the NiO2 system reveals a generalized superconducting dome characterized by systematic shifts in unit cell volume and electron-hole populations across the lanthanides.
The occurrence of unconventional superconductivity in cuprates has long motivated the search for manifestations in other layered transition metal oxides. Recently, superconductivity is found in infinite-layer nickelate (Nd,Sr)NiO2 and (Pr,Sr)NiO2 thin films, formed by topotactic reduction from the perovskite precursor phase. A topic of much current interest is whether rare-earth moments are essential for superconductivity in this system. In this study, it is found that with significant materials optimization, substantial portions of the La1-xSrxNiO2 phase diagram can enter the regime of coherent low-temperature transport (x = 0.14 - 0.20), with subsequent superconducting transitions and a maximum onset of approximate to 9 K at x = 0.20. Additionally, the unexpected indication of a superconducting ground state in undoped LaNiO2 is observed, which likely reflects the self-doped nature of the electronic structure. Combining the results of (La/Pr/Nd)(1-)xSrxNiO2 reveals a generalized superconducting dome, characterized by systematic shifts in the unit cell volume and in the relative electron-hole populations across the lanthanides.

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