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Kosterlitz-Thouless transition in disordered two-dimensional topological insulators.

Zhong Xu1, L Sheng, R Shen

  • 1National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China.

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Disorder drives a metal-insulator transition in quantum spin Hall systems. This transition is a Kosterlitz-Thouless type, characterized by vortex-antivortex pair dynamics and independent of time-reversal symmetry.

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Area of Science:

  • Condensed matter physics
  • Topological materials
  • Quantum phenomena

Background:

  • Quantum spin Hall (QSH) systems exhibit unique electronic properties due to strong spin-orbit coupling.
  • Disorder can significantly alter the electronic behavior of topological materials, potentially driving phase transitions.
  • Understanding metal-insulator transitions is crucial for characterizing the stability and properties of QSH states.

Purpose of the Study:

  • To investigate the nature of the disorder-driven metal-insulator transition in quantum spin Hall systems.
  • To analyze the role of electron delocalization and critical phenomena in this transition.
  • To determine the universality class of the observed transition.

Main Methods:

  • Scaling analysis of the Thouless conductance (g) with sample size (M).
  • Calculation of the beta function (β = d ln g/d ln M) to characterize the flow of conductance.
  • Identification of critical disorder strength and transition type based on conductance behavior.

Main Results:

  • Below a critical disorder strength, conductance remains independent of sample size, indicating critically delocalized states.
  • The calculated beta function confirms a Kosterlitz-Thouless (KT) type metal-insulator transition.
  • The KT-like transition is driven by the binding and unbinding of local current vortex-antivortex pairs.

Conclusions:

  • The disorder-driven metal-insulator transition in QSH systems is of the Kosterlitz-Thouless type.
  • This transition is a fundamental characteristic of the quantum spin Hall state.
  • The observed KT-like transition is robust and does not depend on time-reversal symmetry.