We present a novel approximation scheme for the treatment of stronglycorrelated electrons in arbitrary crystal lattices. The approach extends thewell-known dynamical mean field theory to include nonlocal two-sitecorrelations of arbitrary spatial extent. We extract the nonlocal correlationfunctions from two-impurity Anderson models where the impurity-impuritydistance defines the spatial extent of the correlations included. Translationalinvariance is fully respected by our approach since correlation functions ofany two-impurity cluster are periodically embedded to $k$-space via a Fouriertransform. As a first application, we study the two-dimensional Hubbard modelon a simple-cubic lattice. We demonstrate how pseudogap formation in themany-body resonance at the Fermi level results from the inclusion of nonlocalcorrelations.
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机译:我们介绍了一种用于治疗任意晶格中的强烈康塞的电子的新近似方案。该方法延伸了已知的动态平均场理论,包括任意空间程度的非识别二架子。我们从两种杂质和谐模型中提取非局部相关罚分,其中杂质 - ImpurityDistance在包括所包括的相关性的空间程度。通过我们的方法完全尊重译立invariance,因为Any Any-Icurity集群的相关函数通过FourierTransform定期嵌入到$ k $ -space。作为第一个应用程序,我们研究了二维哈贝德模型一个简单的立方格格子。我们展示了在FERMI水平的基础内谐振中的PseudoGAP在Fermi水平中形成了伪核素的影响。
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