2018
DOI: 10.5890/jand.2018.03.009
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Dynamics of Three and Four Non-identical Josephson Junctions

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Cited by 7 publications
(9 citation statements)
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“…Parameters of the RLC-load are ε = 0.5, γ = 1, ω 2 0 = 1.2 for both cases. The parameters are taken from [Kuznetsov et al, 2018;Vlasov and Pikovsky, 2013]. We have chosen matrices N 2 and N 3 to be identity matrices of the corresponding sizes.…”
Section: Numerical Simulation Resultsmentioning
confidence: 99%
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“…Parameters of the RLC-load are ε = 0.5, γ = 1, ω 2 0 = 1.2 for both cases. The parameters are taken from [Kuznetsov et al, 2018;Vlasov and Pikovsky, 2013]. We have chosen matrices N 2 and N 3 to be identity matrices of the corresponding sizes.…”
Section: Numerical Simulation Resultsmentioning
confidence: 99%
“…The identical junctions can be described by the system of ordinary differential equations (ODE system) in dimensionless global variables [Kuznetsov et al, 2018;Vlasov and Pikovsky, 2013]:…”
Section: Identical Josephson Junctions Array Modelmentioning
confidence: 99%
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“…Being the main constituent element of the SQUID (finer magnetic field detector and RSFQ where Josephson junctions act as transistor and would allow to obtain frequencies in hundreds of GHz), the Josephson junction by its physical properties, is a device of choice for several fields of application and is therefore the subject of several studies and scientific research. For example, recently, in January 2018, Nuznetsov et al studied in [18] the dynamics of three and four non-identical Josephson junctions connected in series and coupled with an RLC dipole. Our motivations for this study are also justified by the recently research on the electromechanical systems.…”
Section: Introductionmentioning
confidence: 99%