Chaotic dynamics of resistively coupled DC-driven distinct Josephson junctions and the effects of circuit parameters

dc.authoridKurt, Erol/0000-0002-3615-6926
dc.authorscopusid7006207315
dc.authorscopusid55235432300
dc.authorwosidKurt, Erol/K-2015-2012
dc.contributor.authorKurt, Erol
dc.contributor.authorCanturk, Mehmet
dc.contributor.otherComputer Engineering
dc.date.accessioned2024-07-05T15:12:00Z
dc.date.available2024-07-05T15:12:00Z
dc.date.issued2009
dc.departmentAtılım Universityen_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, Turkeyen_US
dc.descriptionKurt, Erol/0000-0002-3615-6926en_US
dc.description.abstractTwo 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.citation19
dc.identifier.doi10.1016/j.physd.2009.09.005
dc.identifier.endpage2237en_US
dc.identifier.issn0167-2789
dc.identifier.issue22en_US
dc.identifier.scopus2-s2.0-70349783551
dc.identifier.startpage2229en_US
dc.identifier.urihttps://doi.org/10.1016/j.physd.2009.09.005
dc.identifier.urihttps://hdl.handle.net/20.500.14411/1524
dc.identifier.volume238en_US
dc.identifier.wosWOS:000271686000007
dc.identifier.wosqualityQ1
dc.institutionauthorCantürk, Mehmet
dc.language.isoenen_US
dc.publisherElsevier Science Bven_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectJosephson junctionen_US
dc.subjectDC-drivenen_US
dc.subjectLyapunov exponenten_US
dc.subjectHyper-chaosen_US
dc.titleChaotic dynamics of resistively coupled DC-driven distinct Josephson junctions and the effects of circuit parametersen_US
dc.typeArticleen_US
dspace.entity.typePublication
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