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Path-integral Representation For Quantum Spin Models: Application To The Quantum Cavityrnmethod And Monte Carlo Simulations

机译:量子自旋模型的路径积分表示:在量子腔法和蒙特卡洛模拟中的应用

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摘要

The cavity method is a well-established technique for solving classical spin models on sparse random graphs (mean-field models with finite connectivity). Laumann et al. [Phys. Rev. B 78, 134424 (2008)] proposed recently an extension of this method to quantum spin-1/2 models in a transverse field, using a discretized Suzuki-Trotter imaginary-time formalism. Here we show how to take analytically the continuous imaginary-time limit. Our main technical contribution is an explicit procedure to generate the spin trajectories in a path-integral representation of the imaginary-time dynamics. As a side result we also show how this procedure can be used in simple heat bath Monte Carlo simulations of generic quantum spin models. The replica symmetric continuous-time quantum cavity method is formulated for a wide class of models and applied as a simple example on the Bethe lattice ferromagnet in a transverse field. The results of the methods are confronted with various approximation schemes in this particular case. On this system we performed quantum Monte Carlo simulations that confirm the exactness of the cavity method in the thermodynamic limit.
机译:腔法是一种成熟的技术,用于解决稀疏随机图上的经典自旋模型(具有有限连通性的平均场模型)。劳曼等。 [物理Rev. B 78,134424(2008)]最近提出了使用离散Suzuki-Trotter虚构时间形式论将该方法扩展到横向场中的量子自旋1/2模型的方法。在这里,我们展示了如何解析连续虚时限。我们的主要技术贡献是显式过程,以虚时动力学的路径积分表示形式生成自旋轨迹。作为附带结果,我们还显示了如何在通用量子自旋模型的简单热浴蒙特卡洛模拟中使用此过程。复制对称连续时间量子腔方法适用于多种模型,并作为简单示例应用于Bethe晶格铁磁体的横向场中。在这种特殊情况下,方法的结果面临着各种近似方案。在此系统上,我们执行了量子蒙特卡洛模拟,以确认腔法在热力学极限内的正确性。

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