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双层石墨烯。双层石墨烯中的化学势和量子霍尔铁磁体。

Bilayer graphene. Chemical potential and quantum Hall ferromagnetism in bilayer graphene.

机构信息

Microelectronics Research Center, The University of Texas at Austin, 10100 Burnet Road, Austin, TX 78758, USA.

National Institute for Materials Science, 1-1 Namiki Tsukuba Ibaraki 305-0044, Japan.

出版信息

Science. 2014 Jul 4;345(6192):58-61. doi: 10.1126/science.1251003.

Abstract

Bilayer graphene has a distinctive electronic structure influenced by a complex interplay between various degrees of freedom. We probed its chemical potential using double bilayer graphene heterostructures, separated by a hexagonal boron nitride dielectric. The chemical potential has a nonlinear carrier density dependence and bears signatures of electron-electron interactions. The data allowed a direct measurement of the electric field-induced bandgap at zero magnetic field, the orbital Landau level (LL) energies, and the broken-symmetry quantum Hall state gaps at high magnetic fields. We observe spin-to-valley polarized transitions for all half-filled LLs, as well as emerging phases at filling factors ν = 0 and ν = ±2. Furthermore, the data reveal interaction-driven negative compressibility and electron-hole asymmetry in N = 0, 1 LLs.

摘要

双层石墨烯具有独特的电子结构,受到各种自由度之间复杂相互作用的影响。我们使用双层石墨烯异质结构来探测其化学势,该异质结构由六方氮化硼介电层隔开。化学势具有非线性的载流子密度依赖性,并具有电子-电子相互作用的特征。这些数据允许直接测量零磁场下电场诱导的能隙、轨道朗道能级 (LL) 能量以及强磁场下非对称量子霍尔态的能隙。我们观察到所有半满 LL 的自旋-谷极化跃迁,以及填充因子 ν = 0 和 ν = ±2 时出现的新相。此外,数据还揭示了 N = 0、1 LL 中相互作用驱动的负压缩性和电子-空穴非对称性。

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