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Spin-waves in the J1aβˆ’J1bβˆ’J2J_{1a}-J_{1b}-J_{2} orthorombic square-lattice Heisenberg models: Application to the iron pnictide materials

Abstract

Motivated by the observation of spatially anisotropic exchange constants in the iron pnictide materials, we study the spin-wave spectra of the J1aβˆ’J1bβˆ’J2J_{1a}-J_{1b}-J_{2} Heisenberg models on a square-lattice with nearest neighbor exchange J1aJ_{1a} along x and J1bJ_{1b} along y axis and a second neighbor exchange J2J_2. We focus on the regime, where the spins order at (Ο€,0\pi,0), and compute the spectra by systematic expansions around the Ising limit. We study both spin-half and spin-one Heisenberg models as well as a range of parameters to cover various cases proposed for the iron pnictide materials. The low-energy spectra have anisotropic spin-wave velocities and are renormalized with respect to linear spin-wave theory by up to 20 percent, depending on parameters. Extreme anisotropy, consisting of a ferromagnetic J1b=βˆ’βˆ£JF∣J_{1b}=- |J_F|, is best distinguished from a weak anisotropy (J1aβ‰ˆJ1b=J1J_{1a}\approx J_{1b}=J_1, J2>J1/2J_2>J_1/2) by the nature of the spin-waves near the wavevectors (0,Ο€0,\pi) or (Ο€,Ο€\pi,\pi). The reported spectra for the pnictide material CaFe2_2As2_2 clearly imply such an extreme anisotropy.Comment: 6 pages, 10 figure

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    Last time updated on 02/01/2020