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Journal of Magnetism and Magnetic Materials

Phase transitions of the frustrated bilayer spin one XY model

Antonio S. T. Pires

Published Dec 30, 2017• 7 citations
Publisher
DOI
10.1016/j.jmmm.2017.12.099

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Abstract The spin-one honeycomb bilayer XY antiferromagnet has been studied taking into account the effect of the next-near neighbor J2 exchange interactions and single-ion easy plane anisotropy, using a flavor wave theory. We found that, at a critical point α C = 13.8 , where α = J ⊥ / J 1 is the ratio between the interlayer J ⊥ to the intralayer near neighbor J1 exchange interaction, the system shows a quantum phase transition from an Neel ordered phase to a paramagnetic phase. The phase diagram at zero temperature is presented.

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The 2D Fully Frustrated XY(FFXY) class of models is shown to contain a new groundstate in addition to the checkerboard groundstate of the standard 2D XY model. The spin configuration of this additional groundstate is obtained and its connection to a broken Z2-symmetry explained. This means that the class of 2D FFXY models belongs within a U(1) ⊗ Z2 ⊗ Z2-symmetry phase-transition representation. The phase diagram is reviewed and the central charges of the four multicritical points described. The implications for the standard 2D FFXY-model are discussed and elucidated, in particular with respect to the long standing controversy concerning the phase transitions of the standard 2D FFXY-model.

International Journal of Modern Physics B•Aug 20, 2009•0 citations
Abstract The spin-one honeycomb bilayer XY antiferromagnet has been studied taking into account the effect of the next-near neighbor J2 exchange interactions and single-ion easy plane anisotropy, using a flavor wave theory. We found that, at a critical point α C = 13.8 , where α = J ⊥ / J 1 is the ratio between the interlayer J ⊥ to the intralayer near neighbor J1 exchange interaction, the system shows a quantum phase transition from an Neel ordered phase to a paramagnetic phase. The phase diagram at zero temperature is presented.
The 2D Fully Frustrated XY(FFXY) class of models is shown to contain a new groundstate in addition to the checkerboard groundstate of the standard 2D XY model. The spin configuration of this additional groundstate is obtained and its connection to a broken Z2-symmetry explained. This means that the class of 2D FFXY models belongs within a U(1) ⊗ Z2 ⊗ Z2-symmetry phase-transition representation. The phase diagram is reviewed and the central charges of the four multicritical points described. The implications for the standard 2D FFXY-model are discussed and elucidated, in particular with respect to the long standing controversy concerning the phase transitions of the standard 2D FFXY-model.