方形晶格上自旋1/2海森堡反铁磁体的有限温度对称张量网络

D. Poilblanc, M. Mambrini, F. Alet
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引用次数: 8

摘要

在张量网络框架内,(正)热密度算子可以用通过辅助自由度耦合的无限投影纠缠对算子(iPEPO)的双层来近似。为了研究方形晶格上自旋-1/2海森堡模型的热性质,我们引入了一组完全自旋- $SU(2)$和晶格- $C_{4v}$对称的现场张量(键维为$D=4$或$D=7$)和基于空泡的虚时间演化算子的Trotter-Suzuki分解。对斑块进行变分优化,使用从单站点角转移矩阵重整化组固定点获得的完整(对于$D=4$)或简单(对于$D=7$)环境。该方法在热力学极限下与量子蒙特卡罗进行了比较。虽然iPEPO自旋相关长度开始偏离逆温度$\beta \gtrsim 2$的确切指数增长,但一旦绘制逆相关长度,各种可观测值的行为就变得相当准确。我们还发现,直接$T=0$变分能量优化提供的结果完全符合$\beta\rightarrow\infty$有限温度数据的极限,从而验证了虚时间演化过程。将该方法推广到受挫模型,并给出了初步结果。
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Finite-temperature symmetric tensor network for spin-1/2 Heisenberg antiferromagnets on the square lattice
Within the tensor network framework, the (positive) thermal density operator can be approximated by a double layer of infinite Projected Entangled Pair Operator (iPEPO) coupled via ancilla degrees of freedom. To investigate the thermal properties of the spin-1/2 Heisenberg model on the square lattice, we introduce a family of fully spin-$SU(2)$ and lattice-$C_{4v}$ symmetric on-site tensors (of bond dimensions $D=4$ or $D=7$) and a plaquette-based Trotter-Suzuki decomposition of the imaginary-time evolution operator. A variational optimization is performed on the plaquettes, using a full (for $D=4$) or simple (for $D=7$) environment obtained from the single-site Corner Transfer Matrix Renormalization Group fixed point. The method is benchmarked by a comparison to quantum Monte Carlo in the thermodynamic limit. Although the iPEPO spin correlation length starts to deviate from the exact exponential growth for inverse-temperature $\beta \gtrsim 2$, the behavior of various observables turns out to be quite accurate once plotted w.r.t the inverse correlation length. We also find that a direct $T=0$ variational energy optimization provides results in full agreement with the $\beta\rightarrow\infty$ limit of finite-temperature data, hence validating the imaginary-time evolution procedure. Extension of the method to frustrated models is described and preliminary results are shown.
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