Source zotero
Authors Kaiwen Chen, Xiangqi Liu, Jiachen Jiao, Muyuan Zou, Chengyu Jiang, Xin Li, Yixuan Luo, Qiong Wu, Ningyuan Zhang, Yanfeng Guo, Lei Shu
Relevance score Not available in this batch.
Primary category Not available in this batch.
Published 2024-06-21
Research paradigm Experimental
Sample form Unknown

Summary

The recently discovered superconductivity with critical temperature 𝑇𝑐 up to 80 K in the double-layer Nickelate La3⁢Ni2⁢O7−𝛿 under pressure has drawn great attention. Here, we report the positive muon spin relaxation (𝜇+⁢SR) study of polycrystalline La3⁢Ni2⁢O6.92 under ambient pressure. Zero-field 𝜇+⁢SR experiments reveal the existence of magnetic order in La3⁢Ni2⁢O6.92 with 𝑇𝑁=154 K. The weak transverse field 𝜇+⁢SR measurements reveal the bulk nature of magnetism. In addition, a small quantity of oxygen deficiencies can greatly broaden the internal magnetic field distribution sensed by muons.

Materials

Methods

  • Positive muon spin relaxation (μ+SR)
  • Weak transverse field μ+SR

Keywords

Highlights

  • Bulk nature of magnetism confirmed by weak transverse field μ+SR.

Conclusions

  • Magnetic order exists in La3Ni2O6.92 with TN=154 K.
  • Oxygen deficiencies greatly broaden the internal magnetic field distribution.

Main claims

  • Bulk commensurate magnetic order (spin density wave) exists in La3Ni2O6.92 at ambient pressure with TN=154 K.
    • Evidence: ZF-μSR spectra show oscillations below 148 K,wTF-μSR shows magnetic volume fraction reaches 90%,Fitting gives TN=154 K from Bfast1 temperature dependence (Eq.2)
  • Oxygen deficiencies broaden the internal magnetic field distribution sensed by muons.
    • Evidence: Bfast2 component with large relaxation rate attributed to oxygen vacancies,Comparison of field distribution calculations with perfect crystal and vacancy model
  • The magnetic structure is consistent with a spin-charge stripe model with moments along c-axis, and the ordered moment is about 0.22-0.42 μB.
    • Evidence: Dipole field calculation reproduces observed field strengths,Muon stopping site analysis

Workflow

  • Sample synthesis — High-quality polycrystalline sample with controlled oxygen deficiency.
    • Materials: La2O3 (99.999%); NiO (99.99%)
    • Methods: Solid-state reaction; Sintering at 1100°C in air for 50h, repeated 3 times
    • Observations: Powder X-ray diffraction confirms orthorhombic structure (space group Amam); TGA gives oxygen content La3Ni2O6.92
  • Physical property characterization — Bulk property measurements do not show clear anomaly at the magnetic transition due to oxygen inhomogeneity.
    • Materials: Polycrystalline pellet
    • Methods: Resistivity (four-probe method); Magnetization (SQUID)
    • Observations: Resistivity shows negative temperature coefficient, no anomaly near 150K; Magnetic susceptibility shows no magnetic phase transition down to 2 K, upturn at low T
  • Muon spin relaxation experiments — Evidence for bulk commensurate magnetic order with TN=154 K.
    • Materials: Polycrystalline La3Ni2O6.92 powder
    • Methods: Zero-field (ZF) and weak transverse field (wTF) μ+SR
    • Observations: ZF-μSR: Below 170 K, exponential decay; below 148 K, oscillations appear; Fourier transform shows multiple internal fields (10 mT, 140 mT, broad 160 mT); wTF-μSR: Oscillating signal decreases with cooling, reaching 90% magnetic volume fraction below 93K
  • Data analysis and interpretation — The magnetic order is commensurate SDW with possible stripe order; oxygen deficiencies significantly affect the internal field distribution.
    • Materials: μSR spectra
    • Methods: Least-squares fitting with Eq.(1) for ZF and Eq.(3) for wTF; MuFinder and CASTEP for muon stopping sites; DipoleCal for internal field calculation
    • Observations: Four magnetic components (three oscillating, one non-oscillating); Critical exponent β=0.26(2) suggests reduced dimensionality; Dipole field calculation consistent with spin-charge stripe model; Oxygen vacancies cause inhomogeneous broadening (Bfast2 component)