Source zotero
Authors Chen Lu, Ming Zhang, Zhiming Pan, Congjun Wu, Fan Yang
Relevance score Not available in this batch.
Primary category Not available in this batch.
Published 2025-08-27
Research paradigm Theoretical
Sample form Unknown

Summary

The bilayer nickelate La3Ni2O7 under pressure has recently emerged as a promising system for high-Tc superconductivity. In this work, we investigate the fate of the superconducting properties in La3Ni2O7 under pressure, focusing on the effects of structural deformation and apical oxygen vacancies. Employing a low-energy effective t-J∥-J⊥ model for the 3d_x2-y2orbitals within the slave-boson mean-field approach, we demonstrate that the pairing strength is significantly enhanced in the high-pressure tetragonal I4/mmm phase compared to the ambient pressure orthorhombic Amam phase. Furthermore, by simulating random configurations of apical oxygen vacancies, we show that oxygen vacancies suppress both pairing strength and superfluid density. These results underscore the critical role of pressure and oxygen stoichiometry in tuning the SC of La3Ni2O7, providing key insights into optimizing its high-Tc behavior.

Materials

Methods

  • slave-boson mean-field approach
  • low-energy effective t-J∥-J⊥ model

Keywords

Highlights

  • Demonstrates significant enhancement of pairing strength in high-pressure tetragonal phase.
  • Shows that oxygen vacancies suppress pairing strength and superfluid density.

Conclusions

  • Pairing strength is significantly enhanced in the high-pressure tetragonal I4/mmm phase compared to the ambient pressure orthorhombic Amam phase.
  • Oxygen vacancies suppress both pairing strength and superfluid density.
  • Pressure and oxygen stoichiometry play critical roles in tuning superconductivity of La3Ni2O7.

Main claims

  • The superconducting pairing strength and Tc in La3Ni2O7 are significantly enhanced in the high-pressure I4/mmm phase compared to the ambient-pressure Amam phase.
    • Evidence: SBMF calculations give Δ⊥ = -1.38×10-2 eV and Tc ≈ 87 K at HP, vs. -2.40×10-3 eV and 15 K at AP
  • Apical oxygen vacancies suppress the superconductivity, reducing both the pairing order parameter and superfluid density.
    • Evidence: Simulations with random vacancies show average Δ⊥ and Tc decreasing with increasing vacancy concentration,Spatial maps show suppression of Δ⊥ at vacancy sites

Workflow

  • model_construction — A minimal effective model captures superconductivity.
    • Materials: Bilayer t-J∥-J⊥ model for La3Ni2O7 3dx2-y2 orbital
    • Methods: Slave-boson mean-field (SBMF) theory; Hopping parameters from DFT
    • Observations: Interlayer pairing Δ⊥ is the dominant order parameter; Δ⊥ is much larger in HP than AP
  • effect_of_pressure — Pressure enhances pairing strength and Tc significantly due to increased interlayer superexchange.
    • Materials: Same model with AP and HP parameters
    • Methods: SBMF for pairing amplitudes and Tc
    • Observations: Δ⊥: -2.40×10-3 eV (AP), -1.38×10-2 eV (HP); Tc: ≈15 K (AP), ≈87 K (HP); Tc decreases with increasing J∥ for fixed J⊥
  • effect_of_apical_oxygen_vacancies — Apical oxygen vacancies suppress superconductivity by reducing interlayer coupling and local electron density.
    • Materials: Bilayer lattice with random apical oxygen vacancies at concentration δ
    • Methods: Real-space SBMF on finite lattice; Introduce zero interlayer hopping/exchange at vacancy sites
    • Observations: Δ⊥ and superfluid density decrease with δ; Local suppression of Δ⊥ near vacancies; Tc drops from ≈0.13t (δ=0) to ≈0.04t (δ=0.15)