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Fractional Conductance in Strongly Interacting 1D Systems
1Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot, Israel 76100.
Physical Review Letters
|August 7, 2019
Summary
Strong electron interactions in clean 1D systems can cause fractional quantized conductance and shot noise, even with time-reversal symmetry. These phenomena depend on Fermi momentum commensurability and interaction strength.
Area of Science:
- Condensed Matter Physics
- Quantum Transport
Background:
- Electron-electron interactions significantly influence quantum transport in low-dimensional systems.
- Time-reversal symmetry often dictates expected transport properties, but exceptions exist.
Purpose of the Study:
- Investigate conditions for fractional quantized conductance and shot noise in 1D systems.
- Explore the role of strong electron-electron interactions and Fermi momentum commensurability.
- Connect theoretical findings to experimental observations in confined electron gases.
Main Methods:
- Utilized Abelian bosonization to analyze the strongly interacting regime.
- Employed a generalization of Luther-Emery refermionization for finite temperature and length effects.
- Examined conditions for commensurability of Fermi momenta and interaction strengths.
Main Results:
- Identified scenarios leading to two-terminal fractional quantized conductance and shot noise.
- Demonstrated these phenomena can occur even when time-reversal symmetry is conserved.
- Found the 2/5(e^2/h) conductance fraction in multiple model configurations.
- Observed conductance returning to integer values at small energy scales.
Conclusions:
- Strong interactions and specific commensurability conditions are key to fractional transport.
- The model provides a theoretical basis for experimental observations of fractional conductance plateaus.
- Disorder plays a role in the observed transport phenomena at low energies.
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