arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2109.04231cond-mat.str-el
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重整化多体微扰论中的格林函数

Green functions in the renormalized many-body perturbation theory

Václav Janiš

摘要:

我回顾了如何使用多体格林函数重整化相关费米子的微扰理论。引入格林函数对静态平均场论进行了系统的动力学修正.重整化通过单粒子和双粒子格林函数的自洽计算进入微扰理论。在Baym-Kadanoff构造中讨论了单粒子自洽性。我们指出一个固有的二分法的Baym-Kadanoff方法在一个和两个粒子的格林函数之间的关系。它们是Schwinger-Dyson方程,直接从生成Luttinger-Ward泛函导出,和沃德恒等式。后者对两粒子不可约顶点施加了严格的限制,并且在Baym-Kadanoff方法中不能保证。没有一个近似理论能够同时服从这两种关系。我进一步讨论了两个粒子的方法与两个粒子的重整化,提供了一种方法来调和Schwinger-Dyson方程和沃德恒等式。临界Bethe-Salpeter方程的两粒子不可约顶点在微扰理论的两粒子重整化中成为生成泛函。在沃德恒等式中使用不可约顶点来确定超过临界点的序参量,并且在代表Schwinger-Dyson方程的顶点的Bethe-Salpeter方程中使用不可约顶点来确定光谱自能,使得来自两个方程的热力学临界行为定性地相同。最后,我讨论了一个静态的平均场近似与重正化的有效相互作用确定自洽,导致定性正确的描述强电子相关杂质和晶格模型。

英文摘要:

I review the way the many-body Green functions are used to renormalize the perturbation theory of correlated fermions. The Green functions are introduced to implement systematically dynamical corrections to the static mean-field theory. The renormalizations enter the perturbation theory via self-consistent evaluations of one-particle and two-particle Green functions. The one-particle self-consistency is discussed within the Baym-Kadanoff construction. We point to an inherent dichotomy of the Baym-Kadanoff approach in the relation between one and two-particle Green functions. They are the Schwinger-Dyson equation, directly derived from the generating Luttinger-Ward functional, and the Ward identity. The latter imposes a severe restriction on the two-particle irreducible vertex and is not guaranteed in the Baym-Kadanoff approach. No approximate theory is capable to obey both relations. I further discuss the two-particle approach with two-particle renormalizations that offers a way to reconcile the Schwinger-Dyson equation and the Ward identity. The two-particle irreducible vertex from the critical Bethe-Salpeter equation becomes a generating functional in the two-particle renormalization of the perturbation theory. The irreducible vertex is used in the Ward identity to determine the order parameter beyond the critical point and in the Bethe-Salpeter equation representing the vertex of the Schwinger-Dyson equation to determine the spectral self-energy in such a way that the thermodynamic critical behavior from both equations is qualitatively the same. Finally, I discuss a static mean-field-like approximation with a renormalized effective interaction determined self-consistently that leads to a qualitatively correct description of strong electron correlations in impurity and lattice models.

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