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A correlation length due to thermally excited unbound vortexlike defects of the coloring also diverges exponentially owing to their core energy.
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A correlation length due to thermally excited unbound vortexlike defects of the coloring also diverges exponentially owing to their core energy.
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Any 3-coloring can be mapped into chiralities { ηi }, not necessarily vice versa; however, if the return map is possible it is unique [modulo a cyclic permuation of (ABC)].
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Any 3-coloring can be mapped into chiralities { ηi }, not necessarily vice versa; however, if the return map is possible it is unique [modulo a cyclic permuation of (ABC)].
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Due to the constraint [Eq. d5], Q is not actually invariant under flips σi →- σi nor is Eq. d9 really local.
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Due to the constraint [Eq.], Q is not actually invariant under flips σi →- σi nor is Eq. really local.
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The out-of-plane Goldstone mode-rigidly rotating the Heisenberg spins about any axis in the spin plane-induces a special soft mode that has zero restoring cost (to all orders). This indicates the soft-mode fluctuations cannot be perfectly described by the coloring-independent terms Q0. Since the Goldstone mode is the same physically as the gradual wandering of the spin plane as a function of r (which the coloring state floats on top of). I believe it is innocuous.
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The out-of-plane Goldstone mode-rigidly rotating the Heisenberg spins about any axis in the spin plane-induces a special soft mode that has zero restoring cost (to all orders). This indicates the soft-mode fluctuations cannot be perfectly described by the coloring-independent terms Q0. Since the Goldstone mode is the same physically as the gradual wandering of the spin plane as a function of r (which the coloring state floats on top of). I believe it is innocuous.
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We could also expand Eq. d4 to the next order in { ηα } and estimate the coefficients of four- η terms by the same analytic steps used in this Rapid Communication to get Jαβ.
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We could also expand Eq. to the next order in { ηα } and estimate the coefficients of four- η terms by the same analytic steps used in this Rapid Communication to get Jαβ.
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