摘要
该研究利用O K边和Ni L边X射线吸收谱,系统表征了无限层镍氧化物La1-xCaxNiO2中未占据态随掺杂和温度的演化。超导出现在x=0.18至0.27区间。在x≈0.20–0.23附近,低能谱权重发生重新分布:Ni 3d主导态减少而O 2p杂化态增加,表明Ni–O共价性出现轨道选择性交叉。该交叉与霍尔系数符号反转恰好重合,并先于更高掺杂时超导临界温度的下降。通过将输运异常和超导穹顶直接关联到可测量的Ni–O轨道重组,该结果向建立无限层镍酸盐统一的轨道分辨相图迈出了关键一步,并为通过杂化调控设计超导电性提供了实用途径。
材料
方法
- X-ray absorption spectroscopy (XAS)
- X-ray linear dichroism (XLD)
- PLD
- Topotactic reduction
关键词
- ni o hybridization
- orbital selective crossover
- superconducting dome
- hall coefficient sign reversal
- electronic reconstruction
- covalency
- hole doping
亮点
- Mapping of doping- and temperature-dependent unoccupied states in La1-xCaxNiO2 using O K-edge and Ni L-edge XAS.
- Identification of an additional O K-edge pre-edge feature 'b' that emerges in the superconducting regime and weakens in the overdoped regime.
- Discovery that the crossover in Ni–O covalency near x≈0.20-0.23 coincides with Hall coefficient sign reversal and precedes Tc reduction.
- Observation of weak X-ray linear dichroism in La-based films, contrasting with stronger dichroism in Nd-based analogues.
- Providing a unified orbital-resolved phase diagram for infinite-layer nickelates linking transport anomalies to orbital redistribution.
- Demonstration that hybridization control may serve as a practical route to engineer superconductivity.
结论
- O2p–Ni3d hybridization remains robust across the doping series of infinite-layer La1-xCaxNiO2.
- In the superconducting regime, an additional spectral feature appears in the O K-edge pre-edge region.
- Across the superconducting window (0.18 ≤ x ≤ 0.27), low-energy spectral weight redistributes: Ni3d-dominated contributions decrease while O2p-hybridized states increase, most rapidly near x ≈ 0.20-0.23.
- This crossover coincides with a sign change in the Hall coefficient, indicating an orbital-selective reorganization beyond simple carrier modulation.
- At higher doping (x > 0.23), the continued growth of O-hybridized character tracks the suppression of Tc, linking the downturn of the superconducting dome to a hybridization-driven electronic evolution.
- Temperature- and doping-dependent Ni L3-edge measurements reveal weak XLD in La-based films, implying smaller anisotropy between in-plane and out-of-plane unoccupied 3d states compared to Nd-based analogues.
- These findings place Ni–O covalency at the centre of electronic-structure changes across the superconducting dome in La-based infinite-layer nickelates.
- The results refine the phase diagram by connecting transport anomalies to orbital redistribution and suggest hybridization control as a practical route for tuning superconducting behavior.
主要论断
- Superconductivity in La1-xCaxNiO2 occurs for 0.18 ≤ x ≤ 0.27.
- 证据: Abstract: 'Superconductivity occurs for 0.18 ≤ x ≤ 0.27.',Full text: Tc data from Ref. [36] and superconducting dome characterization.
- Near x ≈ 0.20-0.23, low-energy spectral weight redistributes: Ni3d-dominated states decrease while O2p-hybridized states increase.
- 证据: Abstract: 'Near x≈0.20-0.23, low-energy spectral weight redistributes: Ni3d-dominated states decrease while O2p-hybridized states increase.',O K-edge and Ni L-edge XAS spectra show doping-dependent intensity variations.
- This orbital-selective crossover coincides with sign reversal of the Hall coefficient and precedes the reduction of Tc at higher doping.
- 证据: Abstract: 'coincides with a sign reversal of the Hall coefficient and precedes the reduction of the superconducting critical temperature at higher doping.',Full text: comparison of XAS trends with transport data from Ref. [36].
- Results provide a key step toward a unified orbital-resolved phase diagram for infinite-layer nickelates and a practical route to engineer superconductivity via hybridization control.
- 证据: Abstract: 'key step toward a unified, orbital-resolved phase diagram… and a practical route to engineer superconductivity via hybridization control.',Full text: concluding remarks linking orbital reorganization to superconducting dome.
研究流程
- sample_preparation — Thin films of La1-xCaxNiO2 were successfully synthesized across the doping range.
- 材料: La1-xCaxNiO3 perovskite precursor films; SrTiO3 (STO) substrate (uncapped)
- 方法: Pulsed laser deposition (PLD); Soft-chemistry topotactic reduction
- 观察: Conversion from perovskite to infinite-layer phase
- xas_measurement — XAS reveals doping- and temperature-dependent evolution of unoccupied states and Ni-O hybridization.
- 材料: La1-xCaxNiO2 thin films
- 方法: O K-edge X-ray absorption spectroscopy (XAS); Ni L-edge XAS; Total electron yield (TEY) mode; Polarization-dependent X-ray linear dichroism (XLD)
- 观察: Pre-peak feature 'a' at ≈530.7 eV in O K-edge; Emergence of feature 'b' near x=0.18, strongest at x=0.23; Ni L3-edge intensity peaks near x=0.18; Weak XLD in La-based films
- data_analysis — Low-energy spectral weight transfers from Ni3d-dominated to O2p-hybridized states with doping, coinciding with Hall sign change.
- 材料: XAS spectra; Transport data (Hall coefficient, Tc) from Ref. [36]
- 方法: Integrated spectral weight analysis (Region I of O K-edge); Peak intensity ratio analysis (Ni L-edge); Temperature differential ΔIT calculation
- 观察: Ni L-edge intensity peaks at x=0.18, then decreases; O K-edge integrated area (Region I) peaks at x=0.23; ΔIT increases with doping up to x=0.23, then decreases; Sign reversal of Hall coefficient near x≈0.20-0.23
- interpretation — Ni-O hybridization-driven electronic reconstruction links transport anomalies to the superconducting dome in infinite-layer nickelates.
- 材料: XAS results; Transport phase diagram; Literature on nickelates and cuprates
- 方法: Comparison of XAS and transport trends; Orbital-selective crossover analysis
- 观察: Orbital reorganization most rapid near x≈0.20-0.23; Tc suppressed at higher doping as O-hybridized character grows; Ni-O covalency central to electronic evolution