摘要
Spin-charge-orbital order in nickelate superconductors
材料
本批次暂无数据。
方法
本批次暂无数据。
关键词
本批次暂无数据。
亮点
本批次暂无数据。
结论
本批次暂无数据。
主要论断
- The magnetic ground state of La3Ni2O7 is a double spin stripe (DS1) order, characterized by ferromagnetic nearest-neighbor and antiferromagnetic second-neighbor in-plane interactions, and strong interlayer antiferromagnetic coupling.
- 证据: DFT+U calculations show DS1 lowest among all 2×2×1 configurations,Fitted exchange: J1=-1.1 meV, J2=6.5 meV, J⊥≈124 meV
- Interlayer magnetic exchange is much larger than intralayer exchange in La3Ni2O7.
- 证据: J⊥ values (≈124 meV) are two orders of magnitude larger than J1/J2
研究流程
- dft_calculations_of_magnetic_configurations — DS1 is the magnetic ground state.
- 材料: La3Ni2O7 and La4Ni3O10 crystal structures
- 方法: DFT+U calculations using VASP; All possible magnetic configurations in 2×2×1 supercells
- 观察: DS1 (double spin stripe) is lowest in energy for La3Ni2O7; Outer layers of La4Ni3O10 prefer DS1, inner layer shows different order
- fitting_of_magnetic_exchange_interactions — Interlayer exchange is much stronger than intralayer; DS1 is stabilized by the combination of FM J1 and AFM J2.
- 材料: Energies of ≈80 non-equivalent magnetic configurations
- 方法: Machine learning fitting of Heisenberg Hamiltonian; Landau expansion for moment dependence
- 观察: J1 ≈ -1.1 meV (FM), J2 ≈ 6.5 meV (AFM), J⊥ ≈ 124 meV (AFM) for U=1 eV; Splitting of exchange paths
- strain_effect_simulation — Strain can alter magnetic ordering.
- 材料: La3Ni2O7 under compressive strain
- 方法: DFT with fixed c and relaxed a,b
- 观察: Zigzag magnetic order becomes ground state under compressive strain