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Thermal phase transition of generalized Heisenberg models for SU(N) spins on square and honeycomb lattices

机译:SU(N)自旋在方形和蜂窝晶格上的广义Heisenberg模型的热相变

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摘要

We investigate thermal phase transitions to a valence-bond solid phase in SU(N) Heisenberg models with four- or six-body interactions on a square or honeycomb lattice, respectively. In both cases, a thermal phase transition occurs that is accompanied by rotational symmetry breaking of the lattice. We perform quantum Monte Carlo calculations in order to clarify the critical properties of the models. The estimated critical exponents indicate that the universality classes of the square- and honeycomb-lattice cases are identical to those of the classical XY model with a Z[4] symmetry-breaking field and the three-state Potts model, respectively. In the square-lattice case, the thermal exponent, ν, monotonically increases as the system approaches the quantum critical point, while the values of the critical exponents, η and γ/ν, remain constant. From a finite-size scaling analysis, we find that the system exhibits weak universality, because the Z[4] symmetry-breaking field is always marginal. In contrast, ν in the honeycomb-lattice case exhibits a constant value, even in the vicinity of the quantum critical point, because the Z[3] field remains relevant in the SU(3) and SU(4) cases.
机译:我们研究在SU(N)Heisenberg模型中热相转变为价键固相,分别在正方形或蜂窝晶格上具有四体或六体相互作用。在两种情况下,都会发生热相变,并伴随着晶格的旋转对称破坏。我们执行量子蒙特卡洛计算,以阐明模型的关键特性。估计的临界指数表明,正方形和蜂窝格情况的普遍性类别分别与具有Z [4]对称破缺场的经典XY模型和三态Potts模型的普遍性类别相同。在方格情况下,当系统接近量子临界点时,热指数ν单调增加,而临界指数η和γ/ν的值保持恒定。从有限大小的缩放分析中,我们发现系统表现出较弱的通用性,因为Z [4]对称破坏场始终是边际的。相反,即使在量子临界点附近,蜂窝格情况下的ν也显示恒定值,这是因为在SU(3)和SU(4)情况下Z [3]场仍然有意义。

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