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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Quantized Transport of ν=2/3 Fractional Quantum Hall Edge with Disordered Superconducting Proximity
Pok Man Tam1, Hao Chen2,3, Biao Lian2
1Princeton University, Princeton Center for Theoretical Science, Princeton, New Jersey 08544, USA.
Quantum Hall edge states near superconductors typically show variable conversion. However, at the 2/3 filling, disorder stabilizes phases with quantized electron-to-hole conversion, offering a new transport signature.
Area of Science:
- Condensed Matter Physics
- Quantum Phenomena
Background:
- Proximity of superconductors (SC) to Quantum Hall edge states usually leads to nonquantized electron-to-hole conversion.
- This is often attributed to nonuniversal SC couplings and disorder effects.
Purpose of the Study:
- Investigate the impact of disordered SC couplings on fractional quantum Hall (FQH) edge states at ν=2/3.
- Explore the possibility of quantized transport signatures beyond Hall conductance.
Main Methods:
- Theoretical analysis of counterpropagating edge modes in FQH states coupled to a superconductor.
- Modeling the effect of disordered SC couplings on edge state reconstruction.
Main Results:
- Disordered SC couplings can stabilize an infinite set of phases in ν=2/3 FQH edge states.
- These phases exhibit quantized electron-to-hole conversion probability.
- A quantized downstream resistance R_{d}=h/(2q_{N}^{2}e^{2}) is predicted, with |q_{N}|=1, 4, 15, etc.
Conclusions:
- Disorder can lead to novel, stable phases in FQH edge states with SC proximity.
- The predicted quantized resistance serves as a distinct signature of these phases.
- Findings may extend to other systems like fractional Chern insulators.
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