Magnetic excitations in ferro-pnictide materials controlled by a quantum critical point into hidden order
arXiv:1002.0891 · doi:10.1103/PhysRevB.82.014505
Abstract
The two-orbital J1-J2 model that describes a square lattice of frustrated spin-1 iron atoms is analyzed within the linear spin-wave approximation and by exact diagonalization over a 4x4 cluster. A quantum critical point (QCP) is identified that separates hidden magnetic order at weak Hund's rule coupling from a commensurate spins density wave (cSDW) at strong Hund's rule coupling. Although the moment for cSDW order is small at the QCP, the critical linear spin-wave spectrum shows strong low-energy excitations centered at the wavenumbers that correspond to cSDW order. These disperse anisotropically. A fit to the magnetic excitation spectrum of ferro-pnictide materials obtained recently by inelastic neutron scattering measurements notably accounts for the absence of softening at the wavenumber that corresponds to Neel order.
20 pages, 8 figures, added discussion on doping, published version
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- Superconductivity by Hidden Spin Fluctuations in Electron-Doped Iron Selenide
- Fermi surface pockets in electron-doped iron superconductor by Lifshitz transition
- Spin Resonances in Iron-Selenide High-Tc Superconductors by Proximity to Hidden Spin Density Wave
- Isotropic Cooper Pairs with Emergent Sign Changes in Single-Layer Iron Superconductor
- Fermi surfaces of iron-pnictide high-Tc superconductors from the limit of local magnetic moments
- Collective Mode at Lifshitz Transition in Iron-Pnictide Superconductors
- Particle-Hole Transformation in Strongly-Doped Iron-Based Superconductors
- Two-orbital quantum spin model of magnetism in the iron pnictides
- Quantum-Critical Spin-Density Waves in Iron-Selenide High-Tc Superconductors