论文标题

Moiré石墨烯中的扭曲角域的运输

Transport across twist angle domains in moiré graphene

论文作者

Padhi, Bikash, Tiwari, Apoorv, Neupert, Titus, Ryu, Shinsei

论文摘要

扭曲的双层石墨烯(TBG)中的许多实验在其相图的细节方面彼此不同。除了几乎没有可控的方面,这种差异在很大程度上被认为是由于不同样品之间存在不同程度的扭曲角度不均匀性而产生的。真实的空间图确实揭示了TBG设备分裂成不同扭曲角度的几个大域。在这些观察结果的激励下,我们研究了跨域壁(DW)的量子机械隧道,该隧道将两个区域分开。我们表明,可以通过在DW处形成有效的步骤电位来理解Moiré颗粒的隧穿。此步骤电位的高度只是衡量扭角差异的量度。这些计算使我们确定用于检测和量化局部扭转角变化的全球运输特征。特别是,使用Landauer-Büttiker形式主义,我们计算单渠道电导($ di/dv $)和FANO因子的射击噪声(噪声功率和平均电流比)。在电导率中观察到零偏置,亚M-EV转运缝隙,该距离尺寸为台阶电位的高度。我们作品的主要发现之一是,在扭曲角度不均匀的情况下运输是“嘈杂的”,尽管是副杂志。特别是,范围的差分范围因子峰附近的范霍夫能量与样品中的域相对应。峰的位置和强度仅仅是扭曲角度不均匀程度的度量。

Many of the experiments in twisted bilayer graphene (TBG) differ from each other in terms of the details of their phase diagrams. Few controllable aspects aside, this discrepancy is largely believed to be arising from the presence of a varying degree of twist angle inhomogeneity across different samples. Real space maps indeed reveal TBG devices splitting into several large domains of different twist angles. Motivated by these observations, we study the quantum mechanical tunneling across a domain wall (DW) that separates two such regions. We show that the tunneling of the moiré particles can be understood by the formation of an effective step potential at the DW. The height of this step potential is simply a measure of the difference in twist angles. These computations lead us to identify the global transport signatures for detecting and quantifying the local twist angle variations. In particular, Using Landauer-Büttiker formalism we compute single-channel conductance ($dI/dV$) and Fano factor for shot noise (ratio of noise power and mean current). A zero-bias, sub-meV transport gap is observed in the conductance which scales with the height of the step potential. One of the key findings of our work is that transport in presence of twist angle inhomogeneity is "noisy", though sub-Poissonian. In particular, the differential Fano factor peaks near the van Hove energies corresponding to the domains in the sample. The location and the strength of the peak is simply a measure of the degree of twist angle inhomogeneity.

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