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Incidentally, the classical system thus obtained is precisely the stochastic matrix form decomposition of the zero-temperature Kitaev model [APNYA6 0003-4916 10.1016/j.aop.2005.01.006
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Incidentally, the classical system thus obtained is precisely the stochastic matrix form decomposition of the zero-temperature Kitaev model [C. Castelnovo, C. Chamon, C. Mudry, and P. Pujol, Ann. Phys. (N.Y.) APNYA6 0003-4916 10.1016/j.aop.2005.01.006 318, 316 (2005)].
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The thermal fragility of the topological order in the 2D Kitaev model was already observed by Nussinov and Ortiz arXiv:cond-mat/0605316; and it was also studied by
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The thermal fragility of the topological order in the 2D Kitaev model was already observed by Nussinov and Ortiz arXiv:cond-mat/0605316; and it was also studied by
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16
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34250182747
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Using the results by PRBMDO 0163-1829 10.1103/PhysRevB.75.214407
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Using the results by Furukawa and Misguich [Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.75.214407 75, 214407 (2007)], one can show that the group condition of Eq. 3 can be dropped in the derivation of Eq. 15.
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A similar notion of separability of the wave function amplitudes has been introduced by PLRAAN 1050-2947 10.1103/PhysRevA.72.012324
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A similar notion of separability of the wave function amplitudes has been introduced by Hamma, [A. Hamma, R. Ionicioiu, and P. Zanardi, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.72.012324 72, 012324 (2005)].
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