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Transport gap in suspended bilayer graphene at zero magnetic field

机译:零磁场下悬浮双层石墨烯的传输间隙

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摘要

We report a change of three orders of magnitude in the resistance of a suspended bilayer graphene flake which varies from a few k Omega in the high-carrier-density regime to several M Omega around the charge neutrality point (CNP). The corresponding transport gap is 8 meV at 0.3 K. The sequence of quantum Hall plateaus appearing at filling factor nu = 2 followed by nu = 1 suggests that the observed gap is caused by the symmetry breaking of the lowest Landau level. Investigation of the gap in a tilted magnetic fields indicates that the resistance at the CNP shows a weak linear decrease for increasing total magnetic field. Those observations are in agreement with a spontaneous valley splitting at zero magnetic field followed by splitting of the spins originating from different valleys with increasing magnetic field. Both the transport gap and B field response point toward the spin-polarized layer-antiferromagnetic state as the ground state in the bilayer graphene sample. The observed nontrivial dependence of the gap value on the normal component of B suggests possible exchange mechanisms in the system.
机译:我们报告了悬浮双层石墨烯薄片的电阻变化了三个数量级,从高载流子密度状态下的几千欧米到电荷中性点(CNP)的几兆欧米不等。相应的传输间隙在0.3 K时为8 meV。出现在填充因子nu = 2后紧随nu = 1的量子霍尔高原序列表明,观察到的间隙是由最低Landau能级的对称破坏引起的。对倾斜磁场中间隙的研究表明,CNP处的电阻显示出随总磁场的增加而线性减小的程度。这些观察结果与零磁场下的自发波谷分裂,然后随着磁场的增加而使源自不同波谷的自旋分裂有关。在双层石墨烯样品中,传输间隙和B场响应都指向自旋极化层-反磁态作为基态。观察到的间隙值对B的正常分量的非平凡依赖关系表明系统中可能存在交换机制。

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