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Extension of dynamical mean-field theory by inclusion of nonlocal two-site correlations with variable distance

机译:通过包含具有可变距离的非局部两点相关来扩展动态平均场理论

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摘要

We present an approximation scheme for the treatment of strongly correlated electrons in arbitrary crystal lattices. The approach extends the well-known dynamical mean-field theory to include nonlocal two-site correlations of arbitrary spatial extent. We extract the nonlocal correlation functions from two-impurity Anderson models where the impurity-impurity distance defines the spatial extent of the correlations included. Translational invariance is fully respected by our approach since correlation functions of any two-impurity cluster are periodically embedded to k space via a Fourier transform. As a first application, we study the two-dimensional Hubbard model on a simple-cubic lattice. We demonstrate how pseudogap formation in the many-body resonance at the Fermi level results from the inclusion of nonlocal correlations. A comparison of the spectral function with the dynamical-cluster approximation shows qualitative agreement of high- as well as low-energy features.
机译:我们提出了一种近似方案,用于处理任意晶格中的强相关电子。该方法扩展了众所周知的动态平均场理论,以包含任意空间范围的非局部两点关联。我们从两个杂质的安德森模型中提取非局部相关函数,其中杂质-杂质的距离定义了所包含的相关性的空间范围。我们的方法充分考虑了平移不变性,因为任何两个杂质簇的相关函数都通过傅立叶变换周期性地嵌入到k空间中。作为第一个应用程序,我们研究了简单三次晶格上的二维Hubbard模型。我们证明了费米能级在多体共振中的伪间隙形成是如何由于包含非局部相关性而产生的。频谱函数与动态聚类近似的比较显示了高能量和低能量特征的定性一致性。

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