用约束随机相位近似和约束泛函重整化群研究Emery模型的有效相互作用

Xing-Jie Han, P. Werner, C. Honerkamp
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引用次数: 5

摘要

固体中电子的下折叠低能模型的有效相互作用可以通过积分出费米能级附近远离目标能带的高能量带来获得。在这里,我们应用约束随机相位近似(cRPA)和约束功能重正化群(cfRG)来计算和比较三波段Emery模型的有效相互作用,该模型通常用于研究铜高温超导体,它们可以通过包含所有单环图而超越cRPA。在半带填充时,我们发现有效相互作用随着电荷转移能($\Delta_{dp}$)的增加而增加,并且作为原子间2$p$-3$d$相互作用($U_{dp}$)的函数得到了类似的行为。然而,有效相互作用对$\Delta_{dp}$比对$ U_{dp}$更敏感。对于大多数参数集,与cfRG相比,cRPA中有效的静态相互作用被过度筛选。在动力学平均场理论(DMFT)中求解半填充低能模型。结果表明,尽管存在不同的静态相互作用,但具有cRPA和cfRG相互作用的体系在相似的$\Delta_{dp}$处表现出Mott跃迁。我们还研究了作为掺杂函数的有效相互作用。cfRG的有效相互作用随电子数的增加而减小,与cRPA相反。在空穴掺杂的情况下观察到反屏蔽现象。在所研究的所有情况下,都观察到直接粒子-空穴通道的近似消去。这表明,至少对于现场交互项的向下折叠,可能需要超越cRPA的方法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Investigation of the effective interactions for the Emery model by the constrained random-phase approximation and constrained functional renormalization group
The effective interaction of downfolded low-energy models for electrons in solids can be obtained by integrating out the high energy bands away from the target band near the Fermi level. Here, we apply the constrained random-phase approximation (cRPA) and constrained functional renormalization group (cfRG), which can go beyond cRPA by including all one-loop diagrams, to calculate and compare the effective interactions of the three-band Emery model, which is often used to investigate cuprate high-temperature superconductors. At half band filling, we find that the effective interaction increases as the charge transfer energy ($\Delta_{dp}$) increases and similar behavior is obtained as a function of the interatomic 2$p$-3$d$ interaction ($U_{dp}$). However, the effective interaction is more sensitive to $\Delta_{dp}$ than $ U_{dp}$. For most of the parameter sets, the effective static interaction is overscreened in cRPA compared to cfRG. The low-energy models at half-filling are solved within dynamical mean-field theory (DMFT). The results show that despite the different static interactions, the systems with cRPA and cfRG interaction exhibit a Mott transition at similar values of $\Delta_{dp}$. We also investigate the effective interaction as a function of doping. The cfRG effective interaction decreases as the electron number increases and displays a trend opposite to that of cRPA. Antiscreening is observed for the hole-doped case. For all the cases studied, the near-cancellation of the direct particle-hole channel is observed. This indicates that at least for the downfolding of the onsite interaction terms, methods beyond cRPA may be required.
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