Antiferroquadrupolar order and rotational symmetry breaking in a generalized bilinear-biquadratic model on a square lattice
arXiv:1603.03027 · doi:10.1103/PhysRevLett.118.176401
Abstract
The magnetic and nematic properties of the iron chalcogenides have recently been the subject of intense interest. Motivated by the proposed antiferroquadrupolar and Ising-nematic orders for the bulk FeSe, we study the phase diagram of an generalized bilinear-biquadratic model with multi-neighbor interactions. We find a large parameter regime for a (,0) antiferroquadrupolar phase, showing how quantum fluctuations stabilize it by lifting an infinite degeneracy of certain semiclassical states. Evidence for this C-symmetry-breaking quadrupolar phase is also provided by an unbiased density matrix renormalization group analysis. We discuss the implications of our results for FeSe and related iron-based superconductors.
Finalized version, to appear in PRL
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- Semi-classical simulation of spin-1 magnets
- Possible Nematic Spin Liquid in Spin- Antiferromagnetic System on the Square Lattice: Implication for the Nematic Paramagnetic State of FeSe
- Itinerant approach to magnetic neutron scattering of FeSe: effect of orbital selectivity
- Singular magnetic anisotropy in the nematic phase of FeSe
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