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arXiv 2003.10718cond-mat.stat-mech
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六态时钟模型中相变的纠缠熵研究

Entanglement-entropy study of phase transitions in six-state clock model

Roman Krčmár, Andrej Gendiar, Tomotoshi Nishino

AI总结:

利用角转移矩阵重正化群方法,通过纠缠熵的有限尺寸标度,确定了六态时钟模型的两个BKT相变温度,结果与早期研究一致。

摘要:

通过角转移矩阵重正化群方法研究了正方格子上六态时钟模型的Berezinskii-Kosterlitz-Thouless(BKT)相变。计算了尺寸为$L \ imes L$(最大至$L = 129$)的方形系统的纠缠熵的经典类比量$S( L, T )$,作为温度$T$的函数。该熵在$T = T^*_{~}( L )$处出现峰值,该温度依赖于$L$和边界条件。将有限尺寸标度应用于$T^*_{~}( L )$,并假设存在BKT相变,估计出两个不同的相变温度分别为$T_1^{~} = 0.70$和$T_2^{~} = 0.88$。结果与早期研究一致。值得注意的是,本研究未使用任何热力学函数。

英文摘要:

The Berezinskii-Kosterlitz-Thouless (BKT) transitions of the six-state clock model on the square lattice are investigated by means of the corner-transfer matrix renormalization group method. A classical analog of the entanglement entropy $S( L, T )$ is calculated for $L \times L$ square system up to $L = 129$, as a function of temperature $T$. The entropy exhibits a peak at $T = T^*_{~}( L )$, where the temperature depends on both $L$ and the boundary conditions. Applying the finite-size scaling to $T^*_{~}( L )$ and assuming presence of the BKT transitions, the two distinct phase-transition temperatures are estimated to be $T_1^{~} = 0.70$ and $T_2^{~} = 0.88$. The results are in agreement with earlier studies. It should be noted that no thermodynamic functions have been used in this study.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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