Sheng Feng, Hua Chenqiang, Cheng Man, Hu Jie, Sun Xikang, Tao Qian, Lu Hengzhe, Lu Yunhao, Zhong Mianzeng, Watanabe Kenji, Taniguchi Takashi, Xia Qinglin, Xu Zhu-An, Zheng Yi
Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics, Zhejiang University, Hangzhou, People's Republic of China.
School of Physics and Electronics, Hunan Key Laboratory of Nanophotonics and Devices, Central South University, Changsha, People's Republic of China.
Nature. 2021 May;593(7857):56-60. doi: 10.1038/s41586-021-03449-8. Epub 2021 May 5.
Exciting phenomena may emerge in non-centrosymmetric two-dimensional electronic systems when spin-orbit coupling (SOC) interplays dynamically with Coulomb interactions, band topology and external modulating forces. Here we report synergetic effects between SOC and the Stark effect in centrosymmetric few-layer black arsenic, which manifest as particle-hole asymmetric Rashba valley formation and exotic quantum Hall states that are reversibly controlled by electrostatic gating. The unusual findings are rooted in the puckering square lattice of black arsenic, in which heavy 4p orbitals form a Brillouin zone-centred Γ valley with p symmetry, coexisting with doubly degenerate D valleys of p origin near the time-reversal-invariant momenta of the X points. When a perpendicular electric field breaks the structure inversion symmetry, strong Rashba SOC is activated for the p bands, which produces spin-valley-flavoured D valleys paired by time-reversal symmetry, whereas Rashba splitting of the Γ valley is constrained by the p symmetry. Intriguingly, the giant Stark effect shows the same p-orbital selectiveness, collectively shifting the valence band maximum of the D Rashba valleys to exceed the Γ Rashba top. Such an orchestrating effect allows us to realize gate-tunable Rashba valley manipulations for two-dimensional hole gases, hallmarked by unconventional even-to-odd transitions in quantum Hall states due to the formation of a flavour-dependent Landau level spectrum. For two-dimensional electron gases, the quantization of the Γ Rashba valley is characterized by peculiar density-dependent transitions in the band topology from trivial parabolic pockets to helical Dirac fermions.
当自旋轨道耦合(SOC)与库仑相互作用、能带拓扑结构和外部调制力动态相互作用时,非中心对称二维电子系统中可能会出现令人兴奋的现象。在此,我们报告了中心对称的少层黑砷中SOC与斯塔克效应之间的协同效应,其表现为粒子 - 空穴不对称的 Rashba 谷形成以及可通过静电门控可逆控制的奇异量子霍尔态。这些不同寻常的发现源于黑砷的褶皱方形晶格,其中重的 4p 轨道形成具有 p 对称性的布里渊区中心 Γ 谷,与在 X 点的时间反演不变动量附近起源于 p 的双重简并 D 谷共存。当垂直电场打破结构反演对称性时,p 能带会激活强 Rashba SOC,这会产生由时间反演对称性配对的自旋 - 谷味 D 谷,而 Γ 谷的 Rashba 分裂则受 p 对称性限制。有趣的是,巨大的斯塔克效应表现出相同的 p 轨道选择性,共同将 D Rashba 谷的价带最大值向上移动,使其超过 Γ Rashba 顶部。这种协同效应使我们能够实现对二维空穴气体的门控可调 Rashba 谷操纵,其特征是由于形成了依赖于味的朗道能级谱,量子霍尔态中出现非常规的偶数到奇数跃迁。对于二维电子气体,Γ Rashba 谷的量子化特征是能带拓扑结构中从平凡抛物口袋到螺旋狄拉克费米子的特殊密度依赖跃迁。