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Effects of interaction strength, doping, and frustration on the antiferromagnetic phase of the two-dimensional Hubbard model

机译:交互强度,兴奋剂和挫折对其影响   二维Hubbard模型的反铁磁相

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摘要

Recent quantum-gas microscopy of ultracold atoms and scanning tunnelingmicroscopy of the cuprates reveal new detailed information about doped Mottantiferromagnets, which can be compared with calculations. Using cellulardynamical mean-field theory, we map out the antiferromagnetic (AF) phase of thetwo-dimensional Hubbard model as a function of interaction strength $U$, holedoping $\delta$ and temperature $T$. The N\'eel phase boundary is non-monotonicas a function of $U$ and $\delta$. Frustration induced by second-neighborhopping reduces N\'eel order more effectively at small $U$. The doped AF isstabilized at large $U$ by kinetic energy and at small $U$ by potential energy.The transition between the AF insulator and the doped metallic AF iscontinuous. At large $U$, we find in-gap states similar to those observed inscanning tunneling microscopy. We predict that, contrary to the Hubbard bands,these states are only slightly spin polarized.
机译:最近的超冷原子量子气体显微镜和铜酸盐的扫描隧道显微镜揭示了有关掺杂的Mottantiferroro磁铁的新的详细信息,可以与计算进行比较。使用细胞动力学平均场理论,我们将二维Hubbard模型的反铁磁(AF)阶段绘制为相互作用强度$ U $,空穴掺杂$ \ delta $和温度$ T $的函数。 N \'elel相界是非单调的,是$ U $和$ \ delta $的函数。次近邻跳动引起的挫败感在$ U $较小的情况下更有效地降低了N''elel订单。掺杂的AF通过动能稳定在$ U $上,而势能则稳定在小$ U $。AF绝缘子和掺杂金属AF之间的过渡是连续的。在大的美元,我们发现间隙状态类似于在扫描隧道显微镜中观察到的状态。我们预测,与哈伯德带相反,这些状态仅发生轻微的自旋极化。

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