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Dynamics of coexisting rotating waves in unidirectional rings of bistable Duffing oscillators.
Barba-Franco, J J; Gallegos, A; Jaimes-Reátegui, R; Muñoz-Maciel, J; Pisarchik, A N.
Afiliación
  • Barba-Franco JJ; Departamento de Ciencias Exactas y Tecnología, Centro Universitario de los Lagos, Universidad de Guadalajara, Enrique Díaz de León 1144, Colonia Paseos de la Monta na, 47460 Lagos de Moreno, Jalisco, Mexico.
  • Gallegos A; Departamento de Ciencias Exactas y Tecnología, Centro Universitario de los Lagos, Universidad de Guadalajara, Enrique Díaz de León 1144, Colonia Paseos de la Monta na, 47460 Lagos de Moreno, Jalisco, Mexico.
  • Jaimes-Reátegui R; Departamento de Ciencias Exactas y Tecnología, Centro Universitario de los Lagos, Universidad de Guadalajara, Enrique Díaz de León 1144, Colonia Paseos de la Monta na, 47460 Lagos de Moreno, Jalisco, Mexico.
  • Muñoz-Maciel J; Departamento de Ciencias Exactas y Tecnología, Centro Universitario de los Lagos, Universidad de Guadalajara, Enrique Díaz de León 1144, Colonia Paseos de la Monta na, 47460 Lagos de Moreno, Jalisco, Mexico.
  • Pisarchik AN; Center for Biomedical Technology, Universidad Politécnica de Madrid, Campus de Montegancedo, Pozuelo de Alarcón, 28223 Madrid, Spain.
Chaos ; 33(7)2023 Jul 01.
Article en En | MEDLINE | ID: mdl-37433655
ABSTRACT
We study the dynamics of multistable coexisting rotating waves that propagate along a unidirectional ring consisting of coupled double-well Duffing oscillators with different numbers of oscillators. By employing time series analysis, phase portraits, bifurcation diagrams, and basins of attraction, we provide evidence of multistability on the route from coexisting stable equilibria to hyperchaos via a sequence of bifurcations, including the Hopf bifurcation, torus bifurcations, and crisis bifurcations, as the coupling strength is increased. The specific bifurcation route depends on whether the ring comprises an even or odd number of oscillators. In the case of an even number of oscillators, we observe the existence of up to 32 coexisting stable fixed points at relatively weak coupling strengths, while a ring with an odd number of oscillators exhibits 20 coexisting stable equilibria. As the coupling strength increases, a hidden amplitude death attractor is born in an inverse supercritical pitchfork bifurcation in the ring with an even number of oscillators, coexisting with various homoclinic and heteroclinic orbits. Additionally, for stronger coupling, amplitude death coexists with chaos. Notably, the rotating wave speed of all coexisting limit cycles remains approximately constant and undergoes an exponential decrease as the coupling strength is increased. At the same time, the wave frequency varies among different coexisting orbits, exhibiting an almost linear growth with the coupling strength. It is worth mentioning that orbits originating from stronger coupling strengths possess higher frequencies.

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Chaos Asunto de la revista: CIENCIA Año: 2023 Tipo del documento: Article País de afiliación: México

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Chaos Asunto de la revista: CIENCIA Año: 2023 Tipo del documento: Article País de afiliación: México