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Numerical stabilization of entanglement computation in auxiliary-field quantum Monte Carlo simulations of interacting many-fermion systems

机译:辅助场量子蒙特卡罗仿真互动多费米子系统的纠缠计算数值稳定

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摘要

In the absence of a fermion sign problem, auxiliary-field (or determinantal) quantum Monte Carlo (DQMC) approaches have long been the numerical method of choice for unbiased, large-scale simulations of interacting many-fermion systems. More recently, the conceptual scope of this approach has been expanded by introducing ingenious schemes to compute entanglement entropies within its framework. On a practical level, these approaches, however, suffer from a variety of numerical instabilities that have largely impeded their applicability. Here we report on a number of algorithmic advances to overcome many of these numerical instabilities and significantly improve the calculation of entanglement measures in the zero-temperature projective DQMC approach, ultimately allowing us to reach similar system sizes as for the computation of conventional observables. We demonstrate the applicability of this improved DQMC approach by providing an entanglement perspective on the quantum phase transition from a magnetically ordered Mott insulator to a band insulator in the bilayer square lattice Hubbard model at half filling.
机译:在没有费偶符号问题的情况下,辅助场(或确定的)量子蒙特卡罗(DQMC)方法长期以来一直是无偏的互动,大规模模拟的互动许多费米子系统的首选的数值方法。最近,通过引入巧妙方案来扩展这种方法的概念范围,以计算其框架内的纠缠熵。然而,在实际水平上,这些方法遭受了各种数控稳定性,这主要妨碍了他们的适用性。在这里,我们报告了许多算法的进步,以克服许多这些数值不太稳定性,并显着改善零温度投影DQMC方法中的纠缠措施的计算,最终允许我们达到类似的系统尺寸,以便计算传统观察到的计算。我们通过在半填充的双层方形格子隆巴德模型中从磁性有序的薄片绝缘体到带绝缘体的量子相转变提供纠缠性观点来证明这种改进的DQMC方法的适用性。

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