摘要
本文利用极化分辨电子拉曼散射测量了高质量La3Ni2O7单晶,在150 K以下的密度波转变中观察到显著的、对称性依赖的谱权重重新分布:B1g通道呈现不对称峰,B2g通道呈现对称宽峰,分别对应布里渊区X/Y点附近和对角线方向的电子激发。定量分析提取出两组SDW能隙值,B1g通道能隙约为37.5–40.4 meV(2Δ/kBTc≈5.5–5.9),B2g通道能隙约为23.0 meV(2Δ/kBTc≈3.4),表明前者属中等至强耦合,后者属弱耦合。这种动量选择的各向异性耦合强度无法用简单的弱耦合嵌套理论解释,揭示了非常规SDW源于各向异性电子关联。能隙的温度依赖性明显弱于平均场预期,且B2g通道各向同性与B1g通道弱各向异性也支持两种不同耦合机制的共存。该工作确立了La3Ni2O7中SDW的电子特性,为理解压力下镍酸盐高温超导的涌现提供了微观基础。
材料
方法
- polarization-resolved electronic Raman scattering
- quantitative gap analysis
关键词
- spin density wave (sdw) gap
- anisotropic electronic correlations
- momentum selective gap
- brillouin zone x/y points
亮点
- Establishes electronic character of SDW in La3Ni2O7, providing microscopic foundation for understanding superconductivity under pressure.
结论
- SDW gaps in La3Ni2O7 are momentum-selective with intermediate-to-strong coupling near X/Y points and weaker along diagonal, indicating an unconventional SDW driven by anisotropic electronic correlations.
主要论断
- SDW gaps open in La3Ni2O7 below 150 K with different amplitudes on different Fermi surface regions.
- 证据: Raman spectra show redistribution of spectral weight in B1g and B2g channels below 150 K; fitting yields gap values of ≈37-40 meV (B1g) and ≈23 meV (B2g).
- The SDW coupling is weak along the diagonal direction (B2g) and medium-to-strong near X/Y points (B1g).
- 证据: 2Δ/kT ratios: 3.4 for B2g (weak coupling), 5.5-5.9 for B1g (medium-to-strong coupling); lineshape asymmetry indicates strong correlation in B1g.
- The SDW transition is primarily electronic (spin) rather than lattice-driven.
- 证据: No anomalies in phonon modes across transition; no zone-folded phonons; electronic origin supported by lack of lattice signatures.
研究流程
- sample_growth — Single crystals of La3Ni2O7 were grown.
- 材料: La2O3; NiO; O2
- 方法: high-pressure optical floating zone furnace; solid-state reaction
- 观察: High-qualityLa3Ni2O7 single crystals
- Raman_spectroscopy_measurements — SDW gap opening observed in B1g and B2g channels.
- 材料: single crystals
- 方法: polarization-resolved Raman scattering; confocal geometry; 532 nm laser; Stirling fridge
- 观察: Electronic Raman response in A1g, B1g, B2g channels; Spectral weight redistribution below 150 K in B1g and B2g; No change in A1g
- analysis_and_fitting — Anisotropic SDW gaps with different coupling strengths on different Fermi surface regions.
- 方法: memory function fitting; Tsuneto-Maki function; Lorentzian fitting
- 观察: Gap values: Δ_B1g=37.5-40.4 meV, Δ_B2g=23.0 meV; 2Δ/kT ratios: 5.5-5.9 for B1g, 3.4 for B2g; Weak coupling in B2g, medium-to-strong in B1g