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首页> 外文期刊>Physical review.B.Condensed matter and materials physics >Dynamical mean-field theory of the Anderson-Hubbard model with local and nonlocal disorder in tensor formulation
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Dynamical mean-field theory of the Anderson-Hubbard model with local and nonlocal disorder in tensor formulation

机译:张量配方中局部和非局部紊乱的Anderson-Hubbard模型的动态平均场理论

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摘要

To explore correlated electrons in the presence of local and nonlocal disorder, the Blackman-Esterling-Berk method for averaging over off-diagonal disorder is implemented into dynamical mean-field theory using tensor notation. The impurity model combining disorder and correlations is solved using the recently developed fork tensor-product state solver, which allows one to calculate the single particle spectral functions on the real-frequency axis. In the absence of off-diagonal hopping, we establish exact bounds of the spectral function of the noninteracting Bethe lattice with coordination number Z. In the presence of interaction, the Mott insulating paramagnetic phase of the one-band Hubbard model is computed at zero temperature in alloys with site- and off-diagonal disorder. When the Hubbard U parameter is increased, transitions from an alloy band insulator through a correlated metal into a Mott insulating phase are found to take place.
机译:为了在局部和非局部疾病存在下探讨相关电子,用于使用张量符号的动态平均场理论实现用于平均偏差障碍的Blackman-Esterling-Berk方法。 使用最近开发的叉子张于 - 产品状态求解器解决了组合障碍和相关性的杂质模型,其允许人们计算实际频率轴上的单个粒子谱函数。 在没有非对角线跳跃的情况下,我们建立了具有协调数Z的非交互式贝特晶格的光谱功能的精确界限。在相互作用的存在下,一频带隆巴德模型的Mott绝缘顺磁相在零温度下计算 在具有位点和偏差障碍的合金中。 当船站U参数增加时,发现从合金带绝缘体通过相关金属转换成薄荷的绝缘阶段。

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  • 来源
    《Physical review.B.Condensed matter and materials physics》 |2021年第4期|045127.1-045127.14|共14页
  • 作者单位

    Theoretical Physics Ⅱ Institute of Physics University of Augsburg 86135 Augsburg Germany;

    Kavli Institute of Theoretical Sciences University of Chinese Academy of Sciences Beijing 100190 China;

    Theoretical Physics Ⅲ Center for Electronic Correlations and Magnetism Institute of Physics University of Augsburg 86135 Augsburg Germany Augsburg Center for Innovative Technologies University of Augsburg 86135 Augsburg Germany;

    Department of Physics and Astronomy Middle Tennessee State University Murfreesboro Tennessee 37132 USA;

    Center for Computational Quantum Physics Flatiron Institute 162 5th Avenue New York New York 10010 USA;

    Department of Physics & Astronomy Louisiana State University Baton Rouge Louisiana 70803 USA Center for Computation & Technology Louisiana State University Baton Rouge Louisiana 70803 USA;

    Institute of Theoretical and Computational Physics Graz University of Technology 8010 Graz Austria;

    Institute of Theoretical Physics Faculty of Physics University of Warsaw ulica Pasteura 5 02-093 Warszawa Poland;

    Theoretical Physics Ⅲ Center for Electronic Correlations and Magnetism Institute of Physics University of Augsburg 86135 Augsburg Germany;

    Theoretical Physics Ⅲ Center for Electronic Correlations and Magnetism Institute of Physics University of Augsburg 86135 Augsburg Germany Augsburg Center for Innovative Technologies University of Augsburg 86135 Augsburg Germany;

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