Summary
This paper proposes a microscopic Hamiltonian that faithfully reflects the crystal symmetry of the bilayer nickelate La3Ni2O7 under ambient pressure, addressing its unconventional magnetic order. Large-scale density matrix renormalization group calculations reveal that under a large Hund coupling (J_H), a ((pi/2, pi/2)) spin stripe order emerges due to hidden quasi-one-dimensionality and persists over a range of electron concentrations. In the more symmetric high-pressure regime, when the interlayer antiferromagnetic coupling (J_perp) is sufficiently strong, the model exhibits an enhanced tendency for interlayer pairing. This study unveils the microscopic origin of the diagonal spin stripe order and identifies both the Hund coupling (J_H) and the interlayer coupling (J_perp) as key factors controlling the magnetic order and pairing tendency in La3Ni2O7.
Materials
Methods
- density matrix renormalization group (DMRG)
- microscopic Hamiltonian
Keywords
- spin stripe order
- hund's coupling
- interlayer antiferromagnetic coupling
Highlights
- Hidden quasi-one dimensionality of spin stripe order.
- Indispensable role of Hund's coupling.
Conclusions
- Spin stripe order (π/2,π/2) emerges in La3Ni2O7 with sizable Hund's coupling, and superconducting tendency appears when interlayer antiferromagnetic coupling becomes large under pressure.
Main claims
- A microscopic model with non-uniform hopping and Hund's coupling reproduces the (π/2,π/2) spin stripe order observed in La3Ni2O7.
- Evidence: Full text: DMRG calculations show (π/2,π/2) spin stripe order in the model for t' < t and large U.,Abstract: 'Using state-of-the-art density matrix renormalization group calculations, we show that (π/2,π/2) spin stripe order emerges in our model'
- Superconductivity in La3Ni2O7 requires large interlayer antiferromagnetic coupling, which naturally occurs under pressure.
- Evidence: Abstract: 'Our model exhibits superconducting tendency only when the interlayer antiferromagnetic coupling J⊥ becomes sufficiently large, which naturally occurs under pressure.',Full text: DMRG results show power-law decay of interlayer singlet pairing correlation with exponent Ksc < 2 for J⊥=4t.
- Hund's coupling JH plays an indispensable role in stabilizing the spin stripe order.
- Evidence: Abstract: 'The spin stripe order occurs over a range of electron concentrations, but requires a sizable Hund's coupling JH.',Full text: 'We have confirmed numerically that by taking a smaller JH, one needs a larger U to stabilize the stripe order.'
Workflow
- Model Construction — The model describes the interplay of lattice structure and magnetism in La3Ni2O7.
- Materials: Microscopic Hamiltonian for La3Ni2O7; dx2-y2 and dz2 orbitals; Hund's coupling JH; interlayer coupling J⊥
- Methods: Construction of effective bilayer two-orbital model
- Observations: Model captures strain effects via hopping anisotropy
- DMRG Calculation — DMRG results show (π/2,π/2) spin stripe order emerges when t' < t and U is sufficiently large, and superconductivity appears when J⊥ is large.
- Materials: GPU-accelerated DMRG; System sizes up to 400 sites; Bond dimension up to 20000
- Methods: Density matrix renormalization group (DMRG) calculations; Subspace expansion technique
- Observations: Spin correlation functions F(|ri-rj|); Phase diagrams in t'-U plane for fixed JH
- Phase Diagram Analysis — The spin stripe order requires sizable Hund's coupling, and superconductivity occurs when interlayer coupling is sufficiently large.
- Materials: Phase diagrams from DMRG; Spin correlation functions
- Methods: Identification of spin stripe orders (π/2,π/2) and (π,0); Analysis of superconducting correlations (interlayer singlet pairing)
- Observations: (π/2,π/2) SSO stable when decoupled 1D chains are ferromagnetic; Superconducting power-law decay r-Ksc with Ksc < 2 for large J⊥