Summary
Absence of Ni2/Ni3 charge disproportionation and possible roles of O2 p holes in La3Ni2O7−δ revealed by hard x-ray photoemission spectroscopy
Materials
Methods
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Keywords
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Highlights
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Conclusions
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Main claims
- Ni2+/Ni3+ charge disproportionation is absent in La3Ni2O7-δ; instead the ground state is a d8L-d8 mixture, indicating oxygen 2p holes are important.
- Evidence: Ni 2p HAXPES spectra do not show a double-peak structure with 3–4 eV splitting; the main peak and satellite resemble LaNiO3 (d8L) more than NiO (d8).
- The density wave transition and superconductivity are likely associated with correlated carriers of Ni 3d and O 2p character.
- Evidence: Spectral weight at Fermi level is suppressed even above the density wave transition (150 K), suggesting a pseudogap due to electron-electron or excitonic interactions.
Workflow
- sample_preparation — Sample prepared with known oxygen deficiency.
- Materials: La3Ni2O7-δ polycrystalline sample (δ≈0.07)
- Methods: sol-gel method
- Observations: Clean fracture surface obtained
- haxpes_measurements — HAXPES probes bulk electronic structure.
- Materials: Fractured polycrystalline La3Ni2O7-δ
- Methods: Hard x-ray photoemission spectroscopy (HAXPES) at 6.5 keV; MB Scientific A-1 HE analyzer; Beamline BL12XU SPring-8
- Observations: Wide scan shows La, Ni, O, C peaks; O 1s sharp peak at 529 eV with FWHM 0.75 eV; Ni 2p spectra overlapped with La 3d; after subtraction, resembles NiO and LaNiO3
- spectral_analysis — No charge disproportionation; ground state is d8L-d8 mixture with oxygen 2p holes.
- Materials: HAXPES core-level and valence band spectra
- Methods: Subtraction of La 3d5/2 to isolate Ni 2p3/2; Comparison with reference spectra
- Observations: Ni 2p main peak and satellite match LaNiO3 (d8L) rather than NiO (d8); No double-peak structure indicative of Ni2+/Ni3+ charge disproportionation; Valence band pseudogap: spectral weight at Fermi level close to zero