2017
DOI: 10.1088/1361-6528/aa5643
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Nb/InAs nanowire proximity junctions from Josephson to quantum dot regimes

Abstract: The superconducting proximity effect is probed experimentally in Josephson junctions fabricated with InAs nanowires contacted by Nb leads. Contact transparencies [Formula: see text] are observed. The electronic phase coherence length at low temperatures exceeds the channel length. However, the elastic scattering length is a few times shorter than the channel length. Electrical measurements reveal two regimes of quantum transport: (i) the Josephson regime, characterised by a dissipationless current up to ∼100 n… Show more

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Cited by 22 publications
(19 citation statements)
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“…In Fig. 3(b), a second ABS QD 2 is added to the quantum dot separated by 0.35 meV from QD 1 [28]. At low bias, in the blue region, this yields a pair of resonances most clearly seen in the s 0 region.…”
mentioning
confidence: 96%
“…In Fig. 3(b), a second ABS QD 2 is added to the quantum dot separated by 0.35 meV from QD 1 [28]. At low bias, in the blue region, this yields a pair of resonances most clearly seen in the s 0 region.…”
mentioning
confidence: 96%
“…20,21 Recent works reported Josephson effects at high magnetic fields, sufficient to generate unpaired Majorana bound states. 19,[22][23][24] In this Letter we study the critical current as a function of the magnetic field and gate voltage in nanowire Josephson junctions tuned to the mesoscopic few-mode regime. The junctions consist of InSb weak links and NbTiN superconductor contacts.…”
mentioning
confidence: 99%
“…In the superconducting regime, charge localization gives rise to a strong nonmonotonic behavior of the Josephson current as a function of B due to a Zeeman-induced 0 -p phase transition. Our findings are relevant to experiments aiming at detecting Majorana modes in Josephson junction geometries based on depleted NWs under strong Zeeman fields (28)(29)(30). The anomalous B-field dependence of the critical current, owing to the presence of Majoranas in the 0.52 0.44 0.36 junction (31)(32)(33), may be masked by the localization effects and the Kondo physics discussed here.…”
Section: Discussionmentioning
confidence: 57%