Chaotic Dynamics of Resistively Coupled Dc-Driven Distinct Josephson Junctions and the Effects of Circuit Parameters

dc.authorid Kurt, Erol/0000-0002-3615-6926
dc.authorscopusid 7006207315
dc.authorscopusid 55235432300
dc.authorwosid Kurt, Erol/K-2015-2012
dc.contributor.author Kurt, Erol
dc.contributor.author Canturk, Mehmet
dc.contributor.other Computer Engineering
dc.date.accessioned 2024-07-05T15:12:00Z
dc.date.available 2024-07-05T15:12:00Z
dc.date.issued 2009
dc.department Atılım University en_US
dc.department-temp [Kurt, Erol] Gazi Univ, Dept Elect Educ, Fac Tech Educ, TR-06500 Ankara, Turkey; [Canturk, Mehmet] Atilim Univ, Fac Engn, Dept Comp Engn, TR-06836 Ankara, Turkey en_US
dc.description Kurt, Erol/0000-0002-3615-6926 en_US
dc.description.abstract Two distinct Josephson junctions (JJs) connected with a constant coupling resistance R(cp) are theoretically considered to investigate the overall dynamics below and above the critical current I(c). The circuit model of the device is driven by two DC current sources, I(1) and I(2). Each junction is characterized by a nonlinear resistive-capacitive junction (NRCSJ). Having constructed the circuit model, time-dependent simulations are carried out for a variety of control parameter sets. Common techniques such as bifurcation diagrams, two-dimensional attractors and Lyapunov exponents are applied for the determination of chaotic as well as periodic dynamics of the superconducting junction devices. According to the findings, two states (namely superconducting and ordinary conducting) are determined as functions of the source currents. The chaotic current which flows through Rcp exhibits a very rich behavior depending on the source currents I(1) and I(2) and junction capacitances C(1) and C(2). The device characteristics are summarized by a number of three-dimensional phase diagrams in the parameter space. In addition, for certain parameters, hyper-chaotic cases with two positive Lyapunov exponents are encountered. In contrast to earlier studies claiming the need for a sinusoidal feeding current for generating a chaotic signal, our circuitry can easily generate one via a DC source. (C) 2009 Elsevier B.V. All rights reserved. en_US
dc.identifier.citationcount 19
dc.identifier.doi 10.1016/j.physd.2009.09.005
dc.identifier.endpage 2237 en_US
dc.identifier.issn 0167-2789
dc.identifier.issue 22 en_US
dc.identifier.scopus 2-s2.0-70349783551
dc.identifier.startpage 2229 en_US
dc.identifier.uri https://doi.org/10.1016/j.physd.2009.09.005
dc.identifier.uri https://hdl.handle.net/20.500.14411/1524
dc.identifier.volume 238 en_US
dc.identifier.wos WOS:000271686000007
dc.identifier.wosquality Q1
dc.institutionauthor Cantürk, Mehmet
dc.language.iso en en_US
dc.publisher Elsevier Science Bv en_US
dc.relation.publicationcategory Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı en_US
dc.rights info:eu-repo/semantics/closedAccess en_US
dc.scopus.citedbyCount 23
dc.subject Josephson junction en_US
dc.subject DC-driven en_US
dc.subject Lyapunov exponent en_US
dc.subject Hyper-chaos en_US
dc.title Chaotic Dynamics of Resistively Coupled Dc-Driven Distinct Josephson Junctions and the Effects of Circuit Parameters en_US
dc.type Article en_US
dc.wos.citedbyCount 20
dspace.entity.type Publication
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