摘要
该研究从巡游视角探讨了双层镍氧化物的超导与磁性。基于对压缩应变薄膜角分辨光电子能谱的紧束缚拟合,作者引入了标准在位排斥相互作用(包括轨道内U、轨道间U′、Hund耦合JH和配对跳跃JP),并通过随机相位近似(RPA)考虑粒子-空穴涨落对这些裸相互作用进行重整,从而得到有效配对相互作用。结果表明,在强Hund耦合区域,s波超导和(π/2, π/2)自旋密度波(SDW)有序是优势基态;而在弱Hund耦合下,d波配对和(π, π)自旋密度波成为主导基态。该结果与先前密度矩阵重正化群(DMRG)研究定性一致,强调了Hund耦合在决定体系超导配对对称性和磁性类型中的关键作用。
材料
方法
- tight binding
- random phase approximation (RPA)
- ARPES
关键词
亮点
- Key role of Hund's coupling in determining nature of superconductivity and magnetism.
- Qualitative consistency with DMRG studies.
结论
- In strong Hund's coupling regime, s-wave superconductivity and (π/2,π/2) SDW order are favored; in weak Hund's coupling, d-wave pairing and (π,π) SDW are leading.
主要论断
- Strong Hund's coupling favors s-wave superconductivity and (π/2,π/2) SDW order; weaker Hund's coupling favors d-wave pairing and (π,π) SDW
- 证据: From abstract: 'In the strong Hund's coupling regime, we find that s-wave superconductivity and (π/2,π/2) SDW order are the favored ground states. With weaker Hund's coupling, we find that d-wave pairing and (π,π) SDW are the leading ground states'
- Results are qualitatively consistent with DMRG studies, highlighting key role of Hund's coupling
- 证据: From abstract: 'Our results are qualitatively consistent with earlier DMRG studies, and point to the key role played by Hund's coupling'
研究流程
- model_construction — Two-orbital model with Hund's coupling captures low-energy physics
- 材料: La3Ni2O7 compressively strained thin film
- 方法: tight-binding fit to ARPES data
- 观察: Fermi surface with α and β pockets
- random_phase_approximation_calculations — Strong JH favors s-wave SC and (π/2,π/2) SDW; weak JH favors d-wave and (π,π) SDW
- 材料: Tight-binding model
- 方法: RPA for spin susceptibility and effective pairing interaction
- 观察: leading pairing eigenvalue; gap symmetry; spin susceptibility
- analysis_of_pairing_symmetry_and_magnetism — Hzund's coupling is key determinant of both pairing and magnetic order
- 材料: RPA results
- 方法: Linearized gap equation; Susceptibility peak analysis
- 观察: Phase diagram of pairing symmetry; Magnetic ordering vectors