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磁场诱导拓扑绝缘体纳米带中的螺旋模式和拓扑转变。

Magnetic field-induced helical mode and topological transitions in a topological insulator nanoribbon.

机构信息

Birck Nanotechnology Center, Purdue University, West Lafayette, Indiana 47907, USA.

School of Electrical and Computer Engineering, Purdue University, West Lafayette, Indiana 47907, USA.

出版信息

Nat Nanotechnol. 2016 Apr;11(4):345-51. doi: 10.1038/nnano.2015.293. Epub 2016 Jan 18.

DOI:10.1038/nnano.2015.293
PMID:26780658
Abstract

The spin-helical Dirac fermion topological surface states in a topological insulator nanowire or nanoribbon promise novel topological devices and exotic physics such as Majorana fermions. Here, we report local and non-local transport measurements in Bi2Te3 topological insulator nanoribbons that exhibit quasi-ballistic transport over ∼2 μm. The conductance versus axial magnetic flux Φ exhibits Aharonov-Bohm oscillations with maxima occurring alternately at half-integer or integer flux quanta (Φ0 = h/e, where h is Planck's constant and e is the electron charge) depending periodically on the gate-tuned Fermi wavevector (kF) with period 2π/C (where C is the nanoribbon circumference). The conductance versus gate voltage also exhibits kF-periodic oscillations, anti-correlated between Φ = 0 and Φ0/2. These oscillations enable us to probe the Bi2Te3 band structure, and are consistent with the circumferentially quantized topological surface states forming a series of one-dimensional subbands, which undergo periodic magnetic field-induced topological transitions with the disappearance/appearance of the gapless Dirac point with a one-dimensional spin helical mode.

摘要

在拓扑绝缘体纳米线或纳米带中,螺旋狄拉克费米子拓扑表面态有望实现新型拓扑器件和奇异物理,如马约拉纳费米子。在这里,我们报告了在 Bi2Te3 拓扑绝缘体纳米带中进行的局域和非局域输运测量,这些纳米带表现出长达约 2μm 的弹道输运。电导与轴向磁场 Φ 的关系表现出阿哈罗诺夫-玻姆(Aharonov-Bohm)振荡,其最大值在半整数或整数磁通量子(Φ0=h/e,其中 h 是普朗克常数,e 是电子电荷)处交替出现,这取决于周期性地由栅极调谐费米波矢(kF)决定,周期为 2π/C(其中 C 是纳米带的周长)。电导与栅极电压的关系也表现出 kF 周期性振荡,在 Φ=0 和 Φ0/2 之间呈反相关。这些振荡使我们能够探测 Bi2Te3 的能带结构,并且与周期性地量子化的拓扑表面态形成一系列一维子带一致,这些子带随着无带隙狄拉克点的出现/消失,伴随着一维自旋螺旋模式,经历周期性的磁场诱导拓扑转变。

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