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Quantum phase transition and fractional excitations in a topological insulator thin film with Zeeman and excitonic masses

机译:拓扑中的量子相变和分数激发   绝缘薄膜与塞曼和激子质量

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摘要

We study the zero-temperature phase diagram and fractional excitation when athin film of 3D topological insulator has two competing masses: T- symmetricexciton condensation and T- breaking Zeeman effect. Two topologically distinctphases are identified: in one, the quasiparticles can be viewed as in a quantumspin Hall phase, and in the other a quantum anomalous Hall phase. The vorticesof the exciton order parameter can carry fractional charge and statistics ofelectrons in both phases. When the system undergoes the quantum phasetransition between these two phases, the charges, statistics and the number offermionic zero mode of the excitonic vortices are also changed. We derive theeffective field theory for vortices and external gauge field by directlyintegrating out fermions and present an explicit wave function for thefermionic zero mode localized at the excitonic vortices with or without orbitalmagnetic field. The quantum phase transition can be measured by optical Faradayor Kerr effect experiments, and in closing we discuss the conditions requiredto create the excitonic condensate.
机译:我们研究了当3D拓扑绝缘子的薄膜具有两个竞争质量时的零温度相图和分数激励:T对称激子凝聚和T破裂塞曼效应。确定了两个拓扑上截然不同的阶段:一个阶段中,准粒子可以被视为处于量子自旋霍尔阶段,而另一个阶段中,其被视为量子异常霍尔阶段。激子阶数参数的旋涡可携带分数电荷和两相电子。当系统在这两个相之间进行量子相变时,激子涡旋的电荷,统计量和数量提供离子的零模也将改变。通过直接积分费米子,我们推导出了涡流和外标距场的有效场理论,并给出了存在或不存在轨道磁场的情况下,位于激子涡流处的铁离子零模的显式波函数。可以通过光学法拉第(Faradayor)或Kerr效应实验来测量量子相变,最后我们讨论了产生激子冷凝物的条件。

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