Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/736
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dc.contributor.authorKang, Shivpal Singh-
dc.date.accessioned2016-09-30T13:29:06Z-
dc.date.available2016-09-30T13:29:06Z-
dc.date.issued2015-06-25-
dc.identifier.urihttp://hdl.handle.net/123456789/736-
dc.description.abstractThe non-linear action of the system following equation (4) has a globally fixed stable point at , multiple stability and chaotic regions for a range of its parameter a. The fraction of initial conditions going down to , or its basin stability,and the nature of the basins of attraction go as obtained in figure 4. Under nearest-neighbour coupling scheme the system does not show any regular spatiotemporal behaviour, but for small-world and random networks there is a total spatiotemporal coherence for a range of ε(figure 5(a)-(c)).The system is robust under noise and delay (figure 5(d)-(h)). The 2D (a)(b(c)6jijijiφφφdiffusive lattice scheme shows a range of patterns from smooth to chimeras tospatio-temporal chaosen_US
dc.description.sponsorshipIISER-Men_US
dc.language.isoenen_US
dc.publisherIISER-Men_US
dc.subjectPhysicsen_US
dc.titleSimulation and Analysis of the Coupled Map Lattices with SLMen_US
dc.typeThesisen_US
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