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arXiv 2102.09473cond-mat.mes-hallcond-mat.mtrl-sci
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扭曲双层石墨烯手性哈密顿量约化为$2\ imes2$矩阵算符及魔角平带的物理起源

Reduction of the Twisted Bilayer Graphene Chiral Hamiltonian into a $2\times2$ matrix operator and physical origin of flat-bands at magic angles

Gerardo G. Naumis, Leonardo A. Navarro-Labastida, Enrique Aguilar-Méndez, Abdiel Espinosa-Champo

AI总结:

通过考虑粒子-空穴对称性的哈密顿量重整化,将扭曲双层石墨烯手性哈密顿量约化为$2\ imes2$矩阵算符,揭示魔角平带源于相位挫败效应,并与柔性晶体中的 floppy-mode bands 建立了意想不到的联系。

摘要:

通过考虑粒子-空穴对称性的哈密顿量重整化,扭曲石墨烯双层的 chiral Hamiltonian 被写为一个$2\ imes2$矩阵算符。这产生了一个具有平均场和有效非阿贝尔规范势的有效哈密顿量。所提重整化的作用将零模区域映射到基态。在三角晶格中,零能附近的模式具有反键性质。这导致了与高度简并相关的相位挫败效应,并使平带模式类似于在其他二部晶格中观察到的受限模式。令人惊讶的是,所提的哈密顿量重整化表明,魔角处的平带类似于柔性晶体或玻璃中的 floppy-mode bands,在刚性拓扑理论与魔角扭曲二维异质结构物理之间建立了意想不到的联系。

英文摘要:

The chiral Hamiltonian for twisted graphene bilayers is written as a $2\times2$ matrix operator by a renormalization of the Hamiltonian that takes into account the particle-hole symmetry. This results in an effective Hamiltonian with an average field plus and effective non-Abelian gauge potential. The action of the proposed renormalization maps the zero-mode region into the ground state. Modes near zero energy have an antibonding nature in a triangular lattice. This leads to a phase-frustration effect associated with massive degeneration, and makes flat-bands modes similar to confined modes observed in other bipartite lattices. Suprisingly, the proposed Hamiltonian renormalization suggests that flat-bands at magic angles are akin to floppy-mode bands in flexible crystals or glasses, making an unexpected connection between rigidity topological theory and magic angle twisted two-dimensional heterostructures physics.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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