2017
DOI: 10.1063/1.4995622
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Intrinsically shunted Josephson junctions for electronics applications

Abstract: Conventional Josephson metal-insulator-metal devices are inherently underdamped and exhibit hysteretic current-voltage response due to a very high subgap resistance compared to that in the normal state. At the same time, overdamped junctions with single-valued characteristics are needed for most superconducting digital applications. The usual way to overcome the hysteretic behavior is to place an external low-resistance normal-metal shunt in parallel with each junction.

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Cited by 27 publications
(10 citation statements)
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References 72 publications
(139 reference statements)
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“…To conclude, we note that there are other types of junctions which exhibit self-shunting, have sufficiently high Jc, and rela-tively high IcRN values, e.g., SINIS [47], SNIS [48], [49], etc., see a recent review [50]. However, discussion of their pros and cons goes beyond the scope of this manuscript because we are not considering them for the use in our fabrication processes.…”
Section: B Nb/si:nb/nb Josephson Junctionsmentioning
confidence: 99%
“…To conclude, we note that there are other types of junctions which exhibit self-shunting, have sufficiently high Jc, and rela-tively high IcRN values, e.g., SINIS [47], SNIS [48], [49], etc., see a recent review [50]. However, discussion of their pros and cons goes beyond the scope of this manuscript because we are not considering them for the use in our fabrication processes.…”
Section: B Nb/si:nb/nb Josephson Junctionsmentioning
confidence: 99%
“…As can be seen in Figure (c), the differential resistance around I sd = 0 is not strictly zero but R 0 ≈ 200 Ω. This is due to the effect of thermal fluctuations in the junction and can be understood in the framework of the theory by Ambegaokar and Halperin. , In fact, the McCumber parameter β c of the junction is β c = ω J τ RC , with ω J = 2 eV c / ℏ the characteristic Josephson frequency ( ℏ is the reduced Planck constant, V c = I c R N , with I c the critical current) and τ RC = R N C the decay time within the RCSJ model. Approximating the junction capacitance C with a parallel plate capacitor model, we obtain β c = 1.2 × 10 –5 ≪ 1 (for details, see the Supporting Information). Thus, the junction is in the overdamped regime, and the nonvanishing junction voltage even in the limit I sd → 0 can be attributed to a phase-slip resistance contribution.…”
Section: Resultsmentioning
confidence: 95%
“…Форма вольт-амперних характеристик та присутність вище згаданих ознак свідчить про одержання цим способом Джозефсонових переходів SNIS-типу. Розроблені технології можуть бути використані для масового виготовлення Джозефсонових SISпереходів з метою їхніх застосувань в сучасній мікроелектроніці [17,18]. Автори вдячні В. І. Шниркову, В. М. Краснову та Т. Голоду за участь в обговоренні результатів.…”
Section: методика вимірюваньunclassified