Mauro Di Marco, Mauro Forti, Giacomo Innocenti, Luca Pancioni, Alberto Tesi
{"title":"Embedding classic chaotic maps in simple discrete-time memristor circuits","authors":"Mauro Di Marco, Mauro Forti, Giacomo Innocenti, Luca Pancioni, Alberto Tesi","doi":"arxiv-2408.16352","DOIUrl":null,"url":null,"abstract":"In the last few years the literature has witnessed a remarkable surge of\ninterest for maps implemented by discrete-time (DT) memristor circuits. This\npaper investigates on the reasons underlying this type of complex behavior. To\nthis end, the papers considers the map implemented by the simplest memristor\ncircuit given by a capacitor and an ideal flux-controlled memristor or an\ninductor and an ideal charge-controlled memristor. In particular, the\nmanuscript uses the DT flux-charge analysis method (FCAM) introduced in a\nrecent paper to ensure that the first integrals and foliation in invariant\nmanifolds of continuous-time (CT) memristor circuits are preserved exactly in\nthe discretization for any step size. DT-FCAM yields a two-dimensional map in\nthe voltage-current domain (VCD) and a manifold-dependent one-dimensional map\nin the flux-charge domain (FCD), i.e., a one-dimensional map on each invariant\nmanifold. One main result is that, for suitable choices of the circuit\nparameters and memristor nonlinearities, both DT circuits can exactly embed two\nclassic chaotic maps, i.e., the logistic map and the tent map. Moreover, due to\nthe property of extreme multistability, the DT circuits can simultaneously\nembed in the manifolds all the dynamics displayed by varying one parameter in\nthe logistic and tent map. The paper then considers a DT memristor\nMurali-Lakshmanan-Chua circuit and its dual. Via DT-FCAM these circuits\nimplement a three-dimensional map in the VCD and a two-dimensional map on each\ninvariant manifold in the FCD. It is shown that both circuits can\nsimultaneously embed in the manifolds all the dynamics displayed by two other\nclassic chaotic maps, i.e., the Henon map and the Lozi map, when varying one\nparameter in such maps. In essence, these results provide an explanation of why\nit is not surprising to observe complex dynamics even in simple DT memristor\ncircuits.","PeriodicalId":501167,"journal":{"name":"arXiv - PHYS - Chaotic Dynamics","volume":"9 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Chaotic Dynamics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.16352","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In the last few years the literature has witnessed a remarkable surge of
interest for maps implemented by discrete-time (DT) memristor circuits. This
paper investigates on the reasons underlying this type of complex behavior. To
this end, the papers considers the map implemented by the simplest memristor
circuit given by a capacitor and an ideal flux-controlled memristor or an
inductor and an ideal charge-controlled memristor. In particular, the
manuscript uses the DT flux-charge analysis method (FCAM) introduced in a
recent paper to ensure that the first integrals and foliation in invariant
manifolds of continuous-time (CT) memristor circuits are preserved exactly in
the discretization for any step size. DT-FCAM yields a two-dimensional map in
the voltage-current domain (VCD) and a manifold-dependent one-dimensional map
in the flux-charge domain (FCD), i.e., a one-dimensional map on each invariant
manifold. One main result is that, for suitable choices of the circuit
parameters and memristor nonlinearities, both DT circuits can exactly embed two
classic chaotic maps, i.e., the logistic map and the tent map. Moreover, due to
the property of extreme multistability, the DT circuits can simultaneously
embed in the manifolds all the dynamics displayed by varying one parameter in
the logistic and tent map. The paper then considers a DT memristor
Murali-Lakshmanan-Chua circuit and its dual. Via DT-FCAM these circuits
implement a three-dimensional map in the VCD and a two-dimensional map on each
invariant manifold in the FCD. It is shown that both circuits can
simultaneously embed in the manifolds all the dynamics displayed by two other
classic chaotic maps, i.e., the Henon map and the Lozi map, when varying one
parameter in such maps. In essence, these results provide an explanation of why
it is not surprising to observe complex dynamics even in simple DT memristor
circuits.