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Amplitude death, oscillation death, and periodic regimes in dynamically coupled Landau–Stuart oscillators with and without distributed delay

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  • Roopnarain, Ryan
  • Roy Choudhury, S.

Abstract

The effects of a distributed ’weak generic kernel’ delay on dynamically coupled Landau–Stuart limit cycle oscillators are considered. The system is closed via the ’linear chain trick’ and the linear stability analysis of the system and conditions for Hopf bifurcations that initiate oscillations are investigated. After reformulation, the effect of the weak generic kernel delay turns out to be mathematically similar to the linear augmentation scheme considered earlier for coupled oscillator systems. For our coupled Landau–Stuart oscillators the distributed delay produces transitions from amplitude death (AD) or oscillation death (OD) to periodic behavior via Hopf Bifurcations, with the delayed limit cycle shrinking or growing as the delay is varied towards or away from the bifurcation point respectively. The transition from AD to OD occurs here via a supercritical pitchfork bifurcation, as also seen previously for some other couplings. In addition, the dynamically coupled Landau–Stuart system has a secondary limit cycle emerging within the OD parameter regime, in contrast to other couplings and systems studied earlier.

Suggested Citation

  • Roopnarain, Ryan & Roy Choudhury, S., 2021. "Amplitude death, oscillation death, and periodic regimes in dynamically coupled Landau–Stuart oscillators with and without distributed delay," Mathematics and Computers in Simulation (MATCOM), Elsevier, vol. 187(C), pages 30-50.
  • Handle: RePEc:eee:matcom:v:187:y:2021:i:c:p:30-50
    DOI: 10.1016/j.matcom.2021.02.006
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    Cited by:

    1. Naz, Sidra & Raja, Muhammad Asif Zahoor & Kausar, Aneela & Zameer, Aneela & Mehmood, Ammara & Shoaib, Muhammad, 2022. "Dynamics of nonlinear cantilever piezoelectric–mechanical system: An intelligent computational approach," Mathematics and Computers in Simulation (MATCOM), Elsevier, vol. 196(C), pages 88-113.

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