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dc.contributor.authorMaaita, Jamal-Odysseas
dc.contributor.authorProusalis, Dimitrios
dc.date.accessioned2025-04-21T10:35:34Z
dc.date.available2025-04-21T10:35:34Z
dc.date.copyright12/9/2024 12:00:00 AM
dc.date.issued2024
dc.identifier.issn1555-1415
dc.identifier.othercnd_020_01_011008.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4306509
dc.description.abstractA nonregular oscillation is not enough to define a system as chaotic. A more in-depth investigation is required to prove the existence of chaotic behavior, which is challenging. Although many scientists use the Lyapunov Characteristic Exponents to detect chaos, it is not the only method. Several scientists have introduced different methods that utilize various properties of dynamical systems. Hidden Attractors may be chaotic or regular. The fact that they have small basins of attraction introduces difficulties in locating and characterizing them. The paper presents four different chaotic indicators based on the evolution of the deviation vectors: the maximal Lyapunov Exponent, the Lyapunov Characteristic Exponents, the Fast Lyapunov Index (FLI), and the Small Alignment Index. It includes their properties and the advantages and disadvantages of each method. Also, it includes the algorithms to calculate them and their implementation in Python. The paper closes with a comparison between the four indices applied to a system with hidden attractors.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleA Comparison Between Four Chaotic Indicators in Systems With Hidden Attractors
dc.typeJournal Paper
dc.journal.volume20
dc.journal.issue1
dc.journal.titleJournal of Computational and Nonlinear Dynamics
dc.identifier.doi10.1115/1.4067010
dc.journal.fristpage11008-1
dc.journal.lastpage11008-12
dc.page12
dc.treeJournal of Computational and Nonlinear Dynamics:;2024:;volume( 020 ):;issue: 001
dc.contenttypeFulltext


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