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Diagrammatic Monte Carlo approach for diagrammatic extensions of dynamical mean-field theory: Convergence analysis of the dual fermion technique

机译:动态平均场理论图解扩展的图解蒙特卡洛方法:双重费米子技术的收敛性分析

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摘要

The dual fermion approach provides a formally exact prescription for calculating properties of a correlated electron system in terms of a diagrammatic expansion around dynamical mean-field theory (DMFT). Most practical implementations, however, neglect higher-order interaction vertices beyond two-particle scattering in the dual effective action and further truncate the diagrammatic expansion in the two-particle scattering vertex to a leading-order or ladder-type approximation. In this work, we compute the dual fermion expansion for the two-dimensional Hubbard model including all diagram topologies with two-particle interactions to high orders by means of a stochastic diagrammatic Monte Carlo algorithm. We benchmark the obtained self-energy against numerically exact diagrammatic determinant Monte Carlo simulations to systematically assess convergence of the dual fermion series and the validity of these approximations. We observe that, from high temperatures down to the vicinity of the DMFT Neel transition, the dual fermion series converges very quickly to the exact solution in the whole range of Hubbard interactions considered (4 ≤ U/t ≤ 12), implying that contributions from higher-order vertices are small. As the temperature is lowered further, we observe slower series convergence, convergence to incorrect solutions, and ultimately divergence. This happens in a regime where magnetic correlations become significant. We find, however, that the self-consistent particle-hole ladder approximation yields reasonable and often even highly accurate results in this regime.
机译:双重费米子方法为围绕动态平均场理论(DMFT)的图解展开式计算相关电子系统的性质提供了形式上精确的处方。但是,大多数实际的实现在双重有效动作中忽略了两粒子散射以外的高阶交互作用顶点,并且进一步将两粒子散射顶点中的图解展开式截断为前导或梯形近似。在这项工作中,我们通过随机图解蒙特卡洛算法,计算了二维哈伯德模型的双费米子展开式,其中包括所有具有两个粒子相互作用到高阶的图拓扑。我们将获得的自能量与数值精确的图形行列式蒙特卡洛模拟进行基准比较,以系统地评估对偶费米子级数的收敛性和这些近似的有效性。我们观察到,从高温到DMFT Neel转变附近,双费米子级数很快收敛到所考虑的整个Hubbard相互作用范围内的精确解(4≤U / t≤12),这表明来自高阶顶点很小。随着温度的进一步降低,我们观察到较慢的序列收敛,收敛到错误的解以及最终出现分歧。这发生在磁相关变得显着的情况下。但是,我们发现,在这种情况下,自洽的粒子-孔梯形逼近可得出合理的,甚至常常是高度准确的结果。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第3期|035152.1-035152.23|共23页
  • 作者单位

    Departement de Physique and Institut quantique, Universite de Sherbrooke, Sherbrooke, Quibec, J1K 2R1, Canada;

    Physics Department, King's College London, Strand, London WC2R 2LS, United Kingdom;

    Mathematical and Algorithmic Sciences Laboratory, France Research Center, Huawei Technologies France SASU,92100 Boulogne-Billancourt, France;

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