Shi Yanmeng, Lee Yongjin, Che Shi, Pi Ziqi, Espiritu Timothy, Stepanov Petr, Smirnov Dmitry, Lau Chun Ning, Zhang Fan
Department of Physics and Astronomy, University of California, Riverside, Riverside, California 91765, USA.
National High Magnetic Field Laboratory, Tallahassee, Florida 32310, USA.
Phys Rev Lett. 2016 Feb 5;116(5):056601. doi: 10.1103/PhysRevLett.116.056601.
Owing to the spin, valley, and orbital symmetries, the lowest Landau level in bilayer graphene exhibits multicomponent quantum Hall ferromagnetism. Using transport spectroscopy, we investigate the energy gaps of integer and fractional quantum Hall (QH) states in bilayer graphene with controlled layer polarization. The state at filling factor ν=1 has two distinct phases: a layer polarized state that has a larger energy gap and is stabilized by high electric field, and a hitherto unobserved interlayer coherent state with a smaller gap that is stabilized by large magnetic field. In contrast, the ν=2/3 quantum Hall state and a feature at ν=1/2 are only resolved at finite electric field and large magnetic field. These results underscore the importance of controlling layer polarization in understanding the competing symmetries in the unusual QH system of BLG.
由于自旋、能谷和轨道对称性,双层石墨烯中的最低朗道能级呈现多分量量子霍尔铁磁性。利用输运光谱,我们研究了具有可控层极化的双层石墨烯中整数和分数量子霍尔(QH)态的能隙。填充因子ν = 1时的态有两个不同的相:一个具有较大能隙且在高电场下稳定的层极化态,以及一个迄今未观察到的具有较小能隙且在强磁场下稳定的层间相干态。相比之下,ν = 2/3量子霍尔态和ν = 1/2处的一个特征仅在有限电场和强磁场下才能分辨出来。这些结果强调了在理解双层石墨烯异常量子霍尔系统中竞争对称性时控制层极化的重要性。