1996
DOI: 10.1103/physrevb.53.365
|View full text |Cite
|
Sign up to set email alerts
|

Quasiparticle current in ballistic constrictions with finite transparencies of interfaces

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

6
78
0

Year Published

1999
1999
2024
2024

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 93 publications
(84 citation statements)
references
References 23 publications
6
78
0
Order By: Relevance
“…The assumption of an induced hard gap is justified if the SC-NW interface is in the tunneling regime. This seems to be a reasonable assumption since the experimentally reported induced gaps are much smaller than the parent bulk SC gaps [24][25][26], a fact that typically occurs in low-transmittance interfaces [34,36,37] (As a word of caution, the experimental evidence for this identification is still limited and other explanations cannot be completely ruled out). In the tunneling regime, the quantity γ i = ρ 0 t 2…”
mentioning
confidence: 99%
“…The assumption of an induced hard gap is justified if the SC-NW interface is in the tunneling regime. This seems to be a reasonable assumption since the experimentally reported induced gaps are much smaller than the parent bulk SC gaps [24][25][26], a fact that typically occurs in low-transmittance interfaces [34,36,37] (As a word of caution, the experimental evidence for this identification is still limited and other explanations cannot be completely ruled out). In the tunneling regime, the quantity γ i = ρ 0 t 2…”
mentioning
confidence: 99%
“…2(a) for temperatures in the range from 2 to 7 K. The distinct peak and the lowering of dV /dI at its lower bias side can be attributed to the onset of multiple Andreev reflection. 20,21 The relatively small decrease of differential resistance at the lower bias side of the peak by about 10% compared to the higher bias side can be attributed to the presence of an interface barrier. 20,21 As can be seen in Fig.…”
mentioning
confidence: 99%
“…20,21 The relatively small decrease of differential resistance at the lower bias side of the peak by about 10% compared to the higher bias side can be attributed to the presence of an interface barrier. 20,21 As can be seen in Fig. 2(b) (inset), more structures are found in the differential resistance by approaching zero bias.…”
mentioning
confidence: 99%
“…In Fig. 6b, the differential resistance dV/dI as a function of the bias voltage is plotted at temperatures from 2 to 8 K. The distinct peaks at 2 and 3 K, are recognized as the result from Andreev reflection under a superconducting state [43,44], in which electrons/holes will be reflected from the interfaces of junction. The Andreev reflection and resultant excess conductance originates from the interfaces in Sn/CNT/Sn junctions of Sn@CNT NRs.…”
Section: Superconductivity Of Sn@cnt Nrs Below T Cmentioning
confidence: 99%