2010
DOI: 10.1103/physrevb.82.045432
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Control of the transmission phase in an asymmetric four-terminal Aharonov-Bohm interferometer

Abstract: Phase sensitivity and thermal dephasing in coherent electron transport in quasi-one-dimensional ͑1D͒ waveguide rings of an asymmetric four-terminal geometry are studied by magnetotransport measurements. We demonstrate the electrostatic control of the phase in Aharonov-Bohm resistance oscillations and investigate the impact of the measurement circuitry on decoherence. Phase rigidity is broken due to the ring geometry: orthogonal waveguide cross junctions and 1D leads minimize reflections and resonances between … Show more

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Cited by 24 publications
(32 citation statements)
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References 45 publications
(102 reference statements)
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“…() and a full characterization of the phase‐coherent quantum transport in such four‐terminal asymmetric quantum rings is given in Ref. . As shown in Section , a heating current raises Te in the “heater” with respect to the bath temperature, which was set either to Tbath=1.4 K or to Tbath=4.2K.…”
Section: Resultsmentioning
confidence: 99%
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“…() and a full characterization of the phase‐coherent quantum transport in such four‐terminal asymmetric quantum rings is given in Ref. . As shown in Section , a heating current raises Te in the “heater” with respect to the bath temperature, which was set either to Tbath=1.4 K or to Tbath=4.2K.…”
Section: Resultsmentioning
confidence: 99%
“…This leads to the conclusion that in this system the electron–phonon coupling does not yield significant contribution to the heat flow. In previous works , the electron dephasing in quasi‐1D quantum interferometers was investigated with respect to the increase of the lattice temperature. The relation νfalse(Tlatfalse)=ν0eαTlat was shown to hold, with the visibility ν and the fitting parameter α.…”
Section: Discussionmentioning
confidence: 99%
“…Reflections at the cross‐junctions of the leads can also result in the loss of the two‐path interference phase (). Therefore, in order to break the phase rigidity, it is necessary to use multiterminal and asymmetric QRs .…”
Section: Resultsmentioning
confidence: 99%
“…d). This non‐local resistance is sensitive to the transmission phase, due to the multiterminal and asymmetric geometry of the QR . Figure b shows the oscillatory component of the non‐local magnetoresistance R21,34 as a function of B and Vg at T=23 mK.…”
Section: Resultsmentioning
confidence: 99%
“…is determined from the frequency-independent part of the power spectral density of the thermal noise. 10,15 The phase coherence of interfering electrons in a similar device has been characterized before in theory and experiment 16,17 and thermal transport data measured in the same device have been reported. 10,15 The presence of junctions and crossings in a multi-terminal device requires to calculate the electric and thermal transport for the specific sample geometry across a range of Fermi energies.…”
Section: Introductionmentioning
confidence: 99%