首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Interplay of topology and interactions in quantum Hall topological insulators: U(1) symmetry, tunable Luttinger liquid, and interaction-induced phase transitions
【24h】

Interplay of topology and interactions in quantum Hall topological insulators: U(1) symmetry, tunable Luttinger liquid, and interaction-induced phase transitions

机译:量子霍尔拓扑绝缘体中拓扑和相互作用的相互作用:U(1)对称性,可调谐的Luttinger液体以及相互作用引起的相变

获取原文
获取原文并翻译 | 示例
           

摘要

We consider a class of quantum Hall topological insulators: topologically nontrivial states with zero Chern number at finite magnetic field, in which the counterpropagating edge states are protected by a symmetry (spatial or spin) other than time-reversal. HgTe-type heterostructures and graphene are among the relevant systems. We study the effect of electron interactions on the topological properties of the system. We particularly focus on the vicinity of the topological phase transition, marked by the crossing of two Landau levels, where the system is a strongly interacting quantum Hall ferromagnet. We analyze the edge properties using the formalism of the nonlinear σ-model. We establish the symmetry requirement for the topological protection in this interacting system: effective continuous U(1) symmetry with respect to uniaxial isospin rotations must be preserved. If U(1) symmetry is preserved, the topologically nontrivial phase persists; its edge is a helical Luttinger liquid with highly tunable effective interactions. We obtain explicit analytical expressions for the parameters of the Luttinger liquid in the quantum-Hall-ferromagnet regime. However, U(1) symmetry may be broken, either spontaneously or by U(1)-asymmetric interactions. In either case, interaction-induced transitions occur to the respective topologically trivial phases with gapped edge charge excitations.
机译:我们考虑一类量子霍尔拓扑绝缘子:在有限磁场下具有零Chern数的拓扑非平凡状态,其中反向传播的边缘状态受时间反转以外的对称性(空间或自旋)保护。 HgTe型异质结构和石墨烯属于相关系统。我们研究了电子相互作用对系统拓扑特性的影响。我们特别关注拓扑相变的附近,以两个Landau能级的交叉为标志,该系统是一个强相互作用的量子霍尔铁磁体。我们使用非线性σ模型的形式主义来分析边缘属性。我们在此相互作用的系统中建立了拓扑保护的对称性要求:必须保留相对于单轴同位旋旋转的有效连续U(1)对称性。如果保留了U(1)对称性,则拓扑非平凡阶段将继续存在;它的边缘是具有高度可调的有效相互作用的螺旋Luttinger液体。我们获得了在量子霍尔铁磁体系中卢廷格液体参数的明确解析表达式。但是,U(1)对称性可能会自发或通过U(1)-不对称相互作用而被破坏。在任何一种情况下,相互作用引起的跃迁都发生在具有边沿电荷激发的各个拓扑琐碎相中。

著录项

  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2016年第3期|035146.1-035146.24|共24页
  • 作者单位

    Institute for Theoretical Physics and Astrophysics, University of Wuerzburg, 97074 Wuerzburg, Germany;

    Institute for Theoretical Physics and Astrophysics, University of Wuerzburg, 97074 Wuerzburg, Germany;

    Institute for Theoretical Physics and Astrophysics, University of Wuerzburg, 97074 Wuerzburg, Germany;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号