2019
DOI: 10.3390/cryst9070327
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Charging of Superconducting Layers in Arrays of Coupled Josephson Junctions for Overcritical Currents

Abstract: In this work, we effectuated the numerical simulations of the phase dynamics of an array of Josephson junctions taking into account the capacitive coupling between the neighboring junctions and the diffusion current in the stack. We observed that, if we increase the coupling and the dissipation parameters, the IV characteristic changes qualitatively from the IV characteristics studied before. For currents greater than the critical one, we obtained an additional branch in the IV characteristics. This branch is … Show more

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Cited by 5 publications
(4 citation statements)
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“…Second, if the the coupling between the junctions is low, but the dissipation parameter increase over 1, we have another type of IV characteristic without any hysteresis. 5 And in the last case, if the coupling between the junctions is strong enough and the dissipation parameter increase over the critical value specific for this coupling parameter, we can observe branching in the IV characteristic for the overcritical currents.…”
Section: Introductionmentioning
confidence: 84%
See 1 more Smart Citation
“…Second, if the the coupling between the junctions is low, but the dissipation parameter increase over 1, we have another type of IV characteristic without any hysteresis. 5 And in the last case, if the coupling between the junctions is strong enough and the dissipation parameter increase over the critical value specific for this coupling parameter, we can observe branching in the IV characteristic for the overcritical currents.…”
Section: Introductionmentioning
confidence: 84%
“…Theoretical description of the observed phenomena is provided in the article. 5 The additional branch called the traveling wave branch is characterized by lower voltage. More clear, the average voltage on a junction from the stack corresponding to the traveling wave branch is lower than the voltage on a separated junction for the same current.…”
Section: Introductionmentioning
confidence: 99%
“…Until the last decades of the XX century no experimental implementations of Szilard engine were possible, due to the weak development of micro-technologies and low precision of measurement techniques 13 , 14 . However, with the fast development of nanotechnologies 15 17 , enhancement of ion traps technology and implementation of the first quantum computers 18 , the design of the Szilard engine became a practical challenge. Besides the classical schemes of Szilard engine, associated with Maxwell demon, there were proposed memoryless models, where the measurement is used only to localise the particle in its part of the box 19 , 20 .…”
Section: Introductionmentioning
confidence: 99%
“…Until the last decades of the XX century no experimental implementations of Szilard engine were possible, due to the weak development of micro-technologies and low precision of measurement techniques 13,14 . However, with the fast development of nanotechnologies [15][16][17] , enhancement of ion traps technology and implementation of the first quantum computers 18 , the design of the Szilard engine became a practical challenge. Besides the classical schemes of Szilard engine, associated with Maxwell demon, there were proposed memoryless models, where the measurement is used only to localise the particle in its part of the box 19,20 .…”
Section: Introductionmentioning
confidence: 99%