Fractional and integer quantum Hall effects in the zeroth Landau level in graphene

被引:55
作者
Abanin, Dmitry A. [1 ,2 ,3 ]
Feldman, Benjamin E. [1 ]
Yacoby, Amir [1 ]
Halperin, Bertrand I. [1 ]
机构
[1] Harvard Univ, Dept Phys, Cambridge, MA 02138 USA
[2] Perimeter Inst Theoret Phys, Waterloo, ON N2L 6B9, Canada
[3] Inst Quantum Comp, Waterloo, ON N2L 3G1, Canada
来源
PHYSICAL REVIEW B | 2013年 / 88卷 / 11期
基金
美国国家科学基金会;
关键词
SPIN PHASE-TRANSITION; 2-DIMENSIONAL ELECTRON; COMPOSITE FERMIONS; SKYRMIONS; FERROMAGNETS; STATES; CHARGE; NU=2/3;
D O I
10.1103/PhysRevB.88.115407
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Experiments on the fractional quantized Hall effect in the zeroth Landau level of graphene have revealed some striking differences between filling factors in the ranges 0 < vertical bar nu vertical bar < 1 and 1 < vertical bar nu vertical bar < 2. We argue that these differences can be largely understood as a consequence of the effects of terms in the Hamiltonian which break SU(2) valley symmetry, which we find to be important for vertical bar nu vertical bar < 1 but negligible for vertical bar nu vertical bar > 1. The effective absence of valley anisotropy for vertical bar nu vertical bar > 1 means that states with an odd numerator, such as vertical bar nu vertical bar = 5/3 or 7/5, can accommodate charged excitations in the form of large-radius valley skyrmions, which should have a low energy cost and may be easily induced by coupling to impurities. The absence of observed quantum Hall states at these fractions is likely due to the effects of valley skyrmions. For vertical bar nu vertical bar < 1, the anisotropy terms favor phases in which electrons occupy states with opposite spins, similar to the antiferromagnetic state previously hypothesized to be the ground state at nu = 0. The anisotropy and Zeeman energies suppress large-area skyrmions, so that quantized Hall states can be observable at a set of fractions similar to those in GaAs two-dimensional electron systems. In a perpendicular magnetic field B, the competition between the Coulomb energy, which varies as B-1/2, and the Zeeman energy, which varies as B, can explain the observation of apparent phase transitions as a function of B for fixed., as transitions between states with different degrees of spin polarization. In addition to an analysis of various fractional states from this point of view and an examination of the effects of disorder on valley skyrmions, we present new experimental data for the energy gaps at integer fillings nu = 0 and nu = -1, as a function of magnetic field, and we examine the possibility that valley skyrmions may account for the smaller energy gaps observed at nu = -1.
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页数:17
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