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PreprintCC BY-NC-SA 4.0arXiv

Heavily Sr-Doped La2SrNi2O7−δ as a Tetragonal Ruddlesden-Popper Phase at Ambient Pressure

Abstract

High-temperature superconductivity has been found in bilayer Ruddlesden-Popper (RP) nickelates in bulk samples under high pressure, or in thin films via compressive strain. In the superconducting state, a tetragonal structure with a straight Ni-O-Ni bond along c-axis has been commonly observed, together with the suppression or diminishing of the density-wave orders. Therefore, it remains an open question whether these factors are sufficient for achieving superconductivity at ambient pressure. Here we report the first successful synthesis of heavily Sr-doped La2SrNi2O7−δ under high-pressure and high-temperature (HPHT) conditions with a flux method. X-ray diffraction and scanning transmission electron microscopy (STEM) confirm that the material adopts a tetragonal (I4/mmm) structure with an 180∘ Ni-O-Ni bond angle along c-axis. Resistance measurements reveal metallic behavior with a low-temperature upturn and no density-wave features are observed. However, neither pressure nor oxygen variation induces superconductivity. Density functional theory calculations indicate that the holes introduced by Sr doping are predominantly doped into the Ni-3dz2 orbital, leading to the appearance of a very large γ pocket on the Fermi surface at ambient pressure and significantly reducing the occupation of the Ni-3dz2 orbital. Combining the experimental observations with theoretical calculations, we attribute the absence of superconductivity to the serious deviation from the half-filling state of the Ni-3dz2 band, which is crucial for the interlayer antiferromagnetic interaction and thus for pairing. Our work unravels important issues for achieving superconductivity in bilayer nickelate system.

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BibTeX
@misc{zhang2026heavily,
  title = {{Heavily Sr-Doped La$_2$SrNi$_2$O$_7-δ$ as a Tetragonal Ruddlesden-Popper Phase at Ambient Pressure}},
  author = {Yuhang Zhang and Xue Ming and Cui-Qun Chen and Wei Chen and Tian-Yi Li and Zhe-Ning Xiang and Qing Li and Bing-hui Ge and Dao-Xin Yao and Xiyu Zhu and Hai-Hu Wen},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.00542},
  eprint = {2609.00542},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.00542},
  note = {CC BY-NC-SA 4.0},
}
RIS
TY  - UNPB
TI  - Heavily Sr-Doped La_2SrNi_2O_7−δ as a Tetragonal Ruddlesden-Popper Phase at Ambient Pressure
AU  - Yuhang Zhang
AU  - Xue Ming
AU  - Cui-Qun Chen
AU  - Wei Chen
AU  - Tian-Yi Li
AU  - Zhe-Ning Xiang
AU  - Qing Li
AU  - Bing-hui Ge
AU  - Dao-Xin Yao
AU  - Xiyu Zhu
AU  - Hai-Hu Wen
PY  - 2026
DA  - 2026/09/01
PB  - arXiv
DO  - 10.48550/arxiv.2609.00542
UR  - https://arxiv.org/abs/2609.00542
AB  - High-temperature superconductivity has been found in bilayer Ruddlesden-Popper (RP) nickelates in bulk samples under high pressure, or in thin films via compressive strain. In the superconducting state, a tetragonal structure with a straight Ni-O-Ni bond along c-axis has been commonly observed, together with the suppression or diminishing of the density-wave orders. Therefore, it remains an open question whether these factors are sufficient for achieving superconductivity at ambient pressure. Here we report the first successful synthesis of heavily Sr-doped La_2SrNi_2O_7−δ under high-pressure and high-temperature (HPHT) conditions with a flux method. X-ray diffraction and scanning transmission electron microscopy (STEM) confirm that the material adopts a tetragonal (I4/mmm) structure with an 180^∘ Ni-O-Ni bond angle along c-axis. Resistance measurements reveal metallic behavior with a low-temperature upturn and no density-wave features are observed. However, neither pressure nor oxygen variation induces superconductivity. Density functional theory calculations indicate that the holes introduced by Sr doping are predominantly doped into the Ni-3d_z^2 orbital, leading to the appearance of a very large γ pocket on the Fermi surface at ambient pressure and significantly reducing the occupation of the Ni-3d_z^2  orbital. Combining the experimental observations with theoretical calculations, we attribute the absence of superconductivity to the serious deviation from the half-filling state of the Ni-3d_z^2  band, which is crucial for the interlayer antiferromagnetic interaction and thus for pairing. Our work unravels important issues for achieving superconductivity in bilayer nickelate system.
ER  -