Magnon condensation with finite degeneracy on the triangular lattice
arXiv:1312.5935 · doi:10.1103/PhysRevB.89.134425
Abstract
We study the spin 1/2 triangular-lattice -- antiferromagnet close to the saturation field using the dilute Bose gas theory, where the magnetic structure is determined by the condensation of magnons. We focus on the case of ferromagnetic and antiferromagnetic , that is particularly rich because frustration effects allow the single-magnon energy dispersion to have six-fold degenerate minima at incommensurate momenta. Our calculation also includes an interlayer coupling , which covers both antiferromagnetic and ferromagnetic cases including negligibly small regime (two-dimensional case). Besides the spiral and fan phases, we find a new double- phase (superposition of two modes), dubbed "-" (or simply "01") phase, that enjoys a new type of multiferroic character. Certain phase boundaries have a singular dependence for , implying that even a very small interlayer coupling drastically changes the ground state. A mechanism for this singularity is presented. Moreover, in some regions of the parameter space, we show that a dilute gas of magnons can not be stable, and phase separation (corresponding to a magnetization jump) is expected. In the - model (), formation of two-magnon bound states is observed, which can lead to a quadrupolar (spin-nematic) ordered phase. Exact diagonalization analysis is also applied to the search of bound states.
12 pages, 11 figures; v2 48-spin exact diagonalization added, matches published version
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