2015
DOI: 10.1103/physrevb.92.245437
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Topological dephasing in theν=2/3fractional quantum Hall regime

Abstract: We study dephasing in electron transport through a large quantum dot (a Fabry-Perot interferometer) in the fractional quantum Hall regime with filling factor 2/3. In the regime of sequential tunneling, dephasing occurs due to electron fractionalization into counterpropagating charge and neutral edge modes on the dot. In particular, when the charge mode moves much faster than the neutral mode, and at temperatures higher than the level spacing of the dot, electron fractionalization combined with the fractional s… Show more

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Cited by 17 publications
(13 citation statements)
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“…[40]. We mention that a sharp confining potential may also be beneficial for measuring interference at the ν = 1/3 state by preventing edge reconstruction and the proliferation of neutral edge modes [20,47,48] which may cause dephasing [49,50]; neutral modes have been detected at ν = 1/3 and numerous other fractional quantum Hall states in standard GaAs structures without screening wells [51].…”
Section: Fractional Quantum Hall Regimementioning
confidence: 97%
“…[40]. We mention that a sharp confining potential may also be beneficial for measuring interference at the ν = 1/3 state by preventing edge reconstruction and the proliferation of neutral edge modes [20,47,48] which may cause dephasing [49,50]; neutral modes have been detected at ν = 1/3 and numerous other fractional quantum Hall states in standard GaAs structures without screening wells [51].…”
Section: Fractional Quantum Hall Regimementioning
confidence: 97%
“…Additionally, neutral modes have attracted a lot of interest because they carry energy and a quantum number without carrying charge. Moreover, they may drastically suppress anyonic interference [15,16], and are stable in the presence of a noisy environment, with the environment acting to renormalize the edge state tunneling exponents [17,18]. Yet despite the experimental success of Ref.…”
Section: Introductionmentioning
confidence: 99%
“…It follows from Eqs. (48) and (49) that in the case of diffusive heat transport in the outer arms, the effective Fano factor (as defined by Eq. (3)) is super-Poissonian Fano factors, F 1.…”
Section: Outer Arms Line Junctionsmentioning
confidence: 99%
“…46. attributed the loss of interference to proliferation of neutral modes [48,49] induced by edge reconstruction due to a soft edge confinement potential [17,18,47].…”
Section: Introductionmentioning
confidence: 99%