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Symmetric Localization of ν_{tot}=4/3 Fractional Topological Insulator Edges
Yang-Zhi Chou1, Sankar Das Sarma1
1University of Maryland, College Park, Condensed Matter Theory Center and Joint Quantum Institute, Department of Physics, Maryland 20742, USA.
Researchers explored a disordered interacting edge theory for fractional topological insulators at 4/3 filling. They found that edge transport measurements can falsely indicate the absence of these topological states, even when present.
Area of Science:
- Condensed Matter Physics
- Topological Materials
- Quantum Hall Effect
Background:
- Recent experiments on twisted MoTe2 have spurred interest in fractional topological insulators.
- Understanding the edge states of these materials is crucial for their characterization.
Purpose of the Study:
- To develop a disordered interacting edge theory for a fractional topological insulator at nu_tot=4/3.
- To investigate the impact of perturbations on edge state transport and identification.
Main Methods:
- Development of a disordered interacting edge theory for fractional topological insulators.
- Analysis of edge phases and conductance values under S_z-conserving and S_z-changing conditions.
- Exact mapping to a noninteracting fermionic theory exhibiting Anderson localization.
Main Results:
- Three distinct edge phases were identified with possible conductance values of 2/3(e^2/h) and 4/3(e^2/h).
- Interaction-induced insulating edge states can emerge due to S_z-changing perturbations without breaking fundamental symmetries.
- Symmetric Anderson localization can occur regardless of other S_z-conserving perturbations.
Conclusions:
- Edge-state two-terminal transport measurements can lead to false negatives in identifying nu_tot=4/3 fractional topological insulators.
- The study provides an experimentally relevant example of potential misinterpretation of transport data.
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