Umbrella-coplanar transition in the triangular XXZ model with arbitrary spin
arXiv:1510.07969 · doi:10.1103/PhysRevB.93.224402
Abstract
The quantum triangular XXZ model has recently enjoyed a wealth of new theoretical results, especially in relation to the modeling of the BaCoSbO compound. In particular, it has been understood that in a longitudinal magnetic field the umbrella (cone) phase, classically stable in all the easy-plane region of the ground-state phase diagram, is considerably reduced by the effect of quantum fluctuations. We provide more quantitative information for this phenomenon at arbitrary value of the site spin , by employing the dilute Bose gas expansion, valid in the high-field regime; our results improve the available estimates of the expansion. We quantify the extent to which a higher spin suppresses the effect of quantum fluctuations. Besides, we show how in three-dimensional layered systems a relatively small antiferromagnetic interlayer coupling has a similar consequence of bringing back the umbrella phase in some part of the phase diagram.
8 pages, 7 figures; v2 results unchanged, title and abstract slightly modified, introduction expanded, presentation generally improved, references added, matches published version
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- Exact diagonalization and cluster mean-field study of triangular-lattice XXZ antiferromagnets near saturation
- Field-induced decays in triangular-lattice antiferromagnets
- Exact resummation of the Holstein-Primakoff expansion and differential equation approach to operator square-roots
- Quantum spin state transitions in spin-1 equilateral triangular lattice antiferromagnet NaBaNi(PO)
- Continuous control of classical-quantum crossover by external high pressure in the coupled chain compound CsCuCl
- Chiral crossroads in : a tale of frustration in maple leaf lattice
- Non-Coplanar Model States in Quantum Magnetism Applications of the High-Order Coupled Cluster Method
- Quantum many-body scars in the Bose-Hubbard model with a three-body constraint
- Spin Excitation Continuum in the Exactly Solvable Triangular-Lattice Spin Liquid CeMgAl11O19