1982
DOI: 10.1103/physrevb.25.4515
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Transition from metallic to tunneling regimes in superconducting microconstrictions: Excess current, charge imbalance, and supercurrent conversion

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Cited by 3,534 publications
(3,489 citation statements)
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References 13 publications
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“…DC current along the c axis versus voltage (I-V) characteristics (Fig. 2a) reveal excess current below the Bi-2212 T c (~85 K) due to the Andreev reflection at the S-N interfaces 36 , consistent with the model developed for anisotropic superconductors 34 . The observed Andreev reflection indicates that we have achieved a surprisingly low barrier between Bi-2212 and Bi 2 Se 3 .…”
Section: Resultssupporting
confidence: 81%
“…DC current along the c axis versus voltage (I-V) characteristics (Fig. 2a) reveal excess current below the Bi-2212 T c (~85 K) due to the Andreev reflection at the S-N interfaces 36 , consistent with the model developed for anisotropic superconductors 34 . The observed Andreev reflection indicates that we have achieved a surprisingly low barrier between Bi-2212 and Bi 2 Se 3 .…”
Section: Resultssupporting
confidence: 81%
“…Assuming the normal metal to be single band, the previously established quantum waveguide theory (QWT) [5,6] for the wave function matching conditions at the interface is used. While the Blonder Tinkham Klapwijk (BTK) theory [7] predicts a zero energy Andreev bound state (ABS), which is a Majorana fermion (MF) in this case, for each electron pocket, we show that QWT accounts for the correct number of MF's expected from the topological index. The purpose of this work is therefore twofold: (i) as we shall see below, the ABS predicted by QWT correctly reconciles the Andreev problem with the topological index; (ii) we wish to see the interference e ects on the di erential conductance, as the incident electrons go from a single band metal to a multiband superconductor (MBS), as described by QWT theory.…”
Section: Introductionmentioning
confidence: 86%
“…On the contrary, the conductance g s is nite and independent of the disorder parameter Z at the energy value where Eq. (7) is obeyed [5,7,10].…”
Section: The Andreev Problemmentioning
confidence: 99%
“…Природа избыточного тока связана с прохождением куперовских пар под щель сверхпровод-ника в результате андреевской конверсии. Ìежду избыточным то-ком и энергетической щелью существует известное соотношение I exc = q∆/eR N (q ≈ 4/3) [32], где R N -сопротивление контакта при температурах выше T c сверхпроводника.…”
Section: экспериментальная методикаunclassified