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Distinguishing Electronic Band Structure of Single-layer and Bilayer Ruddlesden-Popper Nickelates Probed by in-situ High Pressure X-ray Absorption Near-edge Spectroscopy

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arxiv 2410.04230 v1 pith:CFMX7BI3 submitted 2024-10-05 cond-mat.supr-con cond-mat.str-el

classification cond-mat.supr-concond-mat.str-el
keywords electronicbandbl-la327peakabovepre-edgepressurehole
verification ladder T0 review T1 audit T2 compute T3 formal
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We report a comprehensive study of electronic band structure for single-layer (SL) and bilayer (BL) RP-nickelates probed by in-situ HP X-ray absorption near edge spectroscopy (XANES). At ambient pressure (AP), the energy splitting delta_E of d_3z^2-r^2 and d_x^2-y^2 bands are directly observed in La3Ni2O7 (BL-La327) but not in La2NiO4 (SL-La214) above E_F, underlining the critical role of inner apical O atoms. A combination of DFT-based electronic band structure and projected density of states (PDOS) calculations with simulated XANES enables us to explain the observed main XANES features labelled by a, A, B', B and C when considering the orbital hybridizations, crystal field splitting (CFS) and core-hole screening of different 3d configurations for SL-La214 and BL-La327 nickelates. At high pressure (HP), the delta_E values of pre-edge peak form a dome-like evolution above 7.7 GPa with the maximum locating at around 20 GPa for metallic BL-La327. Analysis of its integrated area and FWHM provides strong evidence that the bonding d_3z^2-r^2 band crosses E_F above about 7.7 GPa for the metallic BL-La327. Growth of integrated area of pre-edge peak and C peak further evidences pressure-induced hole doping effect. Meanwhile, the pressure dependent FWHM of pre-edge peak implies a nonmonotonic evolution of orbital-selective electronic correlation above 7.7 GPa with extrema emerging at about 20 GPa. Moreover, we estimate the relative hole doping level using the energy shift of pre-edge peak, yielding 0.074 hole per Ni site or equivalently 1.1*10^21 cm^-3 at 20 GPa for the metallic BL-La327, which is comparable to cuprates. Our results have timely examined the electronic band structures as obtained from theoretical calculations, emphasizing the essential role of both d_3z^2-r^2 and d_x^2-y^2 bands as well as the electronic correlation in superconducting pairing for pressurized La3Ni2O7.

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Cited by 4 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Local electronic properties of La3Ni2O7 under pressure

    cond-mat.supr-con 2024-12 conditional novelty 7.0 of 10

    Ni ions in La3Ni2O7 remain low-spin (S=1/2) with valence near 2.5+ from ambient conditions up to about 25 GPa and down to 10 K, contradicting several proposed spin-transition explanations.

  2. Origin of the Diagonal Double-Stripe Spin-Density-Wave and Potential Superconductivity in Bulk La$_3$Ni$_2$O$_{7}$ at Ambient Pressure

    cond-mat.supr-con 2024-12 conditional novelty 6.0 of 10

    An RPA analysis of an eight-band tight-binding model for ambient-pressure La3Ni2O7 reproduces the experimentally observed unidirectional diagonal double-stripe spin-density-wave and predicts enhanced pairing under hol...

  3. Spin-density wave and superconductivity in La$_4$Ni$_3$O$_{10}$ under ambient pressure

    cond-mat.supr-con 2024-11 conditional novelty 6.0 of 10

    In La4Ni3O10 at ambient pressure, a stripe spin-density wave with wave vector near (0.7π,0) is driven by Hund's coupling, and hole doping around δ=-0.4 is predicted to induce superconductivity.

  4. Low-temperature mean valence of nickel ions in pressurized La$_3$Ni$_2$O$_7$

    cond-mat.supr-con 2024-12 conditional novelty 4.0 of 10

    Nickel valence in La3Ni2O7 stays close to 2.5+ from ambient pressure to 40 GPa at 20 K, so pressure-induced superconductivity is tied to a structural transition rather than a change in nickel charge.

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