Application of Chaos Induced Near-Resonance Dynamics to Locate the Global Optimum of Functions

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dc.creatorKonnur, Rahul
dc.date2001-07-10
dc.date2001-07-11
dc.date.accessioned2026-07-07T05:33:35Z
dc.date.available2026-07-07T05:33:35Z
dc.descriptionThe problem of locating the global optimum of functions is studied in a dynamic setting. The dynamics of simple multistable systems under the influence of chaotic forcing is investigated. When the magnitude of the forcing signal decays slowly, it is shown that the system attains an equilibrium state, which corresponds to the global optimum of the corresponding multimodal potential function. The role of bifurcations in facilitating the approach to the global optimum is discussed.
dc.description7 Pages,8 Figures
dc.identifierhttps://arxiv.org/abs/nlin/0107017
dc.identifierhttp://arxiv.org/abs/nlin/0107017
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/80044
dc.subjectChaotic Dynamics
dc.titleApplication of Chaos Induced Near-Resonance Dynamics to Locate the Global Optimum of Functions
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