arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2009.09413cond-mat.str-elcond-mat.mes-hallcond-mat.supr-con
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库仑相互作用扭曲双层石墨烯中隐藏对称性的重整化群方法

Towards the hidden symmetry in Coulomb interacting twisted bilayer graphene: renormalization group approach

Oskar Vafek, Jian Kang

摘要:

我们开发了一个两阶段的重整化群,它连接的连续哈密顿量的扭曲双层石墨烯在长度尺度短于莫尔超晶格周期的活性窄带的哈密顿量,这是有效的距离远大于莫尔周期。在第一阶段,库仑相互作用重新规范化的费米速度和层间隧穿,以这样的方式,以抑制相同的亚晶格相反的亚晶格隧穿的比例,因此接近所谓的手征极限。在第二阶段中,层间隧穿被非微扰地处理。通过一个渐进的数值消除远程带的相对强度的单粒子的色散和相互作用内的活性窄带哈密顿量被确定,从而量化的剩余相关性和证明强耦合的方法在最后一步。我们还精确地计算了从库仑相互作用投影到重整化窄带上的激子能谱。所得到的集体模式的软化标志着魔角扭曲双层石墨烯中放大的(“隐藏的”)$U(4)\times U(4)$对称性的接近。

英文摘要:

We develop a two stage renormalization group which connects the continuum Hamiltonian for twisted bilayer graphene at length scales shorter than the moire superlattice period to the Hamiltonian for the active narrow bands only which is valid at distances much longer than the moire period. In the first stage, the Coulomb interaction renormalizes the Fermi velocity and the interlayer tunnelings in such a way as to suppress the ratio of the same sublattice to opposite sublatice tunneling, hence approaching the so-called chiral limit. In the second stage, the interlayer tunneling is treated non-perturbatively. Via a progressive numerical elimination of remote bands the relative strength of the one-particle-like dispersion and the interactions within the active narrow band Hamiltonian is determined, thus quantifying the residual correlations and justifying the strong coupling approach in the final step. We also calculate exactly the exciton energy spectrum from the Coulomb interactions projected onto the renormalized narrow bands. The resulting softening of the collective modes marks the propinquity of the enlarged ("hidden") $U(4)\times U(4)$ symmetry in the magic angle twisted bilayer graphene.

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