Magnetic Field-Controlled Electrical Conductivity in AA Bilayer Graphene

C Pub Date : 2023-04-21 DOI:10.3390/c9020042
Vardan Apinyan, Tadeusz Kopeć
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Abstract

We consider the effect of the external magnetic field on the in-plane conductivity in the AA-stacked bilayer graphene system in the strong excitonic condensate regime. We include the effects of the applied inter-layer electric field and the Coulomb interactions. The on-site and inter-layer Coulomb interactions were treated via the bilayer Hubbard model. Using the solutions for the physical parameters in the system, we calculate the in-plane conductivity of the bilayer graphene. By employing the Green-Kubo formalism for the polarization function in the system, we show that the conductivity in the AA bilayer system is fully controlled by the applied magnetic field. For the partial filling in the layers, the electrical conductivity is different for different spin orientations, and, at the high values of the magnetic field, only one component remains with the given spin orientation. Meanwhile, for the half-filling limit, there is no spin-splitting observed in the conductivity function. The theory evaluated here shows the new possibility for spin-controlled electronic transport in the excitonic bilayer graphene system.
AA双层石墨烯的磁场控制电导率
研究了在强激子凝聚态下,外加磁场对aa堆叠双层石墨烯体系面内电导率的影响。我们包括施加层间电场和库仑相互作用的影响。通过双层Hubbard模型处理现场和层间库仑相互作用。利用系统中物理参数的解,我们计算了双层石墨烯的面内电导率。利用Green-Kubo的极化函数形式,证明了AA双层体系的电导率完全受外加磁场的控制。对于部分填充层,不同自旋取向的电导率是不同的,并且在磁场高值时,只有一个分量保持给定的自旋取向。同时,在半填充极限下,电导率函数没有出现自旋分裂现象。本文所评估的理论显示了在激子双层石墨烯体系中自旋控制电子输运的新可能性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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