Phase diagram of the ?=2 quantum Hall state in bilayer graphene

被引:6
作者
Khanna, Udit [1 ]
Huang, Ke [2 ]
Murthy, Ganpathy [3 ]
Fertig, H. A. [4 ]
Watanabe, Kenji [5 ]
Taniguchi, Takashi [6 ]
Zhu, Jun [2 ]
Shimshoni, Efrat [1 ]
机构
[1] Bar Ilan Univ, Dept Phys, IL-52900 Ramat Gan, Israel
[2] Penn State Univ, Dept Phys, University Pk, PA 16802 USA
[3] Univ Kentucky, Dept Phys & Astron, Lexington, KY 40506 USA
[4] Indiana Univ, Dept Phys, Bloomington, IN 47405 USA
[5] Natl Inst Mat Sci, Res Ctr Funct Mat, 1-1 Namiki, Tsukuba 3050044, Japan
[6] Natl Inst Mat Sci, Int Ctr Mat Nanoarchitecton, 1-1 Namiki, Tsukuba 3050044, Japan
基金
美国国家科学基金会; 以色列科学基金会;
关键词
BROKEN-SYMMETRY; SPIN;
D O I
10.1103/PhysRevB.108.L041107
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Bilayer graphene exhibits a rich phase diagram in the quantum Hall regime, arising from a multitude of internal degrees of freedom, including spin, valley, and orbital indices. The variety of fractional quantum Hall states between filling factors 1 < v = 2 suggests, among other things, a quantum phase transition between valleyunpolarized and polarized states at a perpendicular electric-field D*. We find that the behavior of D* with v changes markedly as B is reduced. At v = 2, D* may even vanish when B is sufficiently small. We present a theoretical model for lattice-scale interactions, which explains these observations; surprisingly, both repulsive and attractive components in the interactions are required. Within this model, we analyze the nature of the v = 2 state as a function of the magnetic and electric fields and predict that valley coherence may emerge for D & SIM; D* in the high-B regime. This suggests the system supports Kekule bond ordering, which could, in principle, be verified via scanning tunneling measurements.
引用
收藏
页数:7
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