Self-consistent spin-wave theory for a frustrated Heisenberg model with biquadratic exchange in the columnar phase and its application to iron pnictides
Daniel Stanek, Oleg P. Sushkov, G\"otz S. Uhrig

TL;DR
This paper extends self-consistent spin-wave theory to a frustrated J1-J2-Jc Heisenberg model with biquadratic exchange, explaining magnetic anisotropy and spin-wave dispersion in iron pnictides, especially CaFe2As2.
Contribution
It introduces mean-field decouplings for biquadratic exchange in the S=1 model and compares Dyson-Maleev and Schwinger boson approaches, providing insights into magnetic anisotropy and excitations.
Findings
Biquadratic exchange enhances anisotropy between spin stripe directions.
The model reproduces spin-wave dispersion in CaFe2As2 perpendicular to spin stripes.
Discrepancies in parallel directions suggest S=2 may be needed for full accuracy.
Abstract
Recent neutron scattering studies revealed the three dimensional character of the magnetism in the iron pnictides and a strong anisotropy between the exchange perpendicular and parallel to the spin stripes. We extend studies of the J1-J2-Jc Heisenberg model with S = 1 using self-consistent spin-wave theory. A discussion of two scenarios for the instability of the columnar phase is provided. The relevance of a biquadratic exchange term between in-plane nearest neighbors is discussed. We introduce mean-field decouplings for biquadratic terms using the Dyson-Maleev and the Schwinger boson representation. Remarkably their respective mean-field theories do not lead to the same results, even at zero temperature. They are gauged in the N'eel phase in comparison to exact diagonalization and series expansion. The J1-J2-Jc model is analyzed under the influence of the biquadratic exchange Jbq and…
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