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Chaos in the fractional order nonlinear Bloch equation with delay

dc.authorwosid Baleanu, Dumitru/B-9936-2012
dc.authorwosid Bhalekar, S./D-7628-2011
dc.contributor.author Baleanu, Dumitru
dc.contributor.author Baleanu, Dumitru
dc.contributor.author Magin, Richard L.
dc.contributor.author Bhalekar, Sachin
dc.contributor.author Daftardar-Gejji, Varsha
dc.contributor.other Matematik
dc.date.accessioned 2017-04-18T11:33:06Z
dc.date.available 2017-04-18T11:33:06Z
dc.date.issued 2015
dc.department Çankaya University en_US
dc.department-temp [Baleanu, Dumitru] Cankaya Univ, Fac Arts & Sci, Dept Math & Comp Sci, TR-06530 Ankara, Turkey; [Baleanu, Dumitru] Inst Space Sci, R-76900 Bucharest, Romania; [Magin, Richard L.] Univ Illinois, Dept Bioengn, Chicago, IL 60607 USA; [Bhalekar, Sachin] Shivaji Univ, Dept Math, Kolhapur 416004, Maharashtra, India; [Daftardar-Gejji, Varsha] Savitribai Phule Pune Univ, Dept Math, Pune 411007, Maharashtra, India en_US
dc.description.abstract The Bloch equation describes the dynamics of nuclear magnetization in the presence of static and time-varying magnetic fields. In this paper we extend a nonlinear model of the Bloch equation to include both fractional derivatives and time delays. The Caputo fractional time derivative (alpha) in the range from 0.85 to 1.00 is introduced on the left side of the Bloch equation in a commensurate manner in increments of 0.01 to provide an adjustable degree of system memory. Time delays for the z component of magnetization are inserted on the right side of the Bloch equation with values of 0, 10 and 100 ms to balance the fractional derivative with delay terms that also express the history of an earlier state. In the absence of delay, tau = 0, we obtained results consistent with the previously published bifurcation diagram, with two cycles appearing at alpha = 0.8548 with subsequent period doubling that leads to chaos at alpha = 0.9436. A periodic window is observed for the range 0.962 < alpha < 0.9858, with chaos arising again as a nears 1.00. The bifurcation diagram for the case with a 10 ms delay is similar: two cycles appear at the value alpha = 0.8532, and the transition from two to four cycles at alpha = 0.9259. With further increases in the fractional order, period doubling continues until at alpha = 0.9449 chaos ensues. In the case of a 100 millisecond delay the transitions from one cycle to two cycles and two cycles to four cycles are observed at alpha = 0.8441, and alpha = 0.8635, respectively. However, the system exhibits chaos at much lower values of a (alpha - 0.8635). A periodic window is observed in the interval 0.897 < alpha < 0.9341, with chaos again appearing for larger values of a. In general, as the value of a decreased the system showed transitions from chaos to transient chaos, and then to stability. Delays naturally appear in many NMR systems, and pulse programming allows the user control over the process. By including both the fractional derivative and time delays in the Bloch equation, we have developed a delay-dependent model that predicts instability in this non-linear fractional order system consistent with the experimental observations of spin turbulence. (C) 2015 Elsevier B.V. All rights reserved. en_US
dc.description.publishedMonth 8
dc.description.sponsorship Shivaji University, Kolhapur, India; Savitribai Phule Pune University, Pune, India en_US
dc.description.sponsorship S. Bhalekar acknowledges Shivaji University, Kolhapur, India for the research grant provided under the Innovative Research Activities. V. Daftardar-Gejji acknowledges Savitribai Phule Pune University, Pune, India for the travel grant to attend the international conference ICFDA14, Catania, Italy. en_US
dc.description.woscitationindex Science Citation Index Expanded
dc.identifier.citation Baleanu, D...et al. (2015). Chaos in the fractional order nonlinear Bloch equation with delay. Communications In Nonlinear Science And Numerical Simulation, 25(1-3), 41-49. http://dx.doi.org/10.1016/j.cnsns.2015.01.004 en_US
dc.identifier.doi 10.1016/j.cnsns.2015.01.004
dc.identifier.endpage 49 en_US
dc.identifier.issn 1007-5704
dc.identifier.issn 1878-7274
dc.identifier.issue 1-3 en_US
dc.identifier.scopusquality Q1
dc.identifier.startpage 41 en_US
dc.identifier.uri https://doi.org/10.1016/j.cnsns.2015.01.004
dc.identifier.volume 25 en_US
dc.identifier.wos WOS:000351075800005
dc.identifier.wosquality Q1
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.subject Bloch Equation en_US
dc.subject Fractional Calculus en_US
dc.subject Chaos en_US
dc.subject Delay en_US
dc.subject Magnetic Resonance en_US
dc.subject Relaxation en_US
dc.title Chaos in the fractional order nonlinear Bloch equation with delay tr_TR
dc.title Chaos in the Fractional Order Nonlinear Bloch Equation With Delay en_US
dc.type Article en_US
dc.wos.citedbyCount 76
dspace.entity.type Publication
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