Localized Patterns in Periodically Forced Systems: II. Patterns with Non-Zero Wavenumber
A. S. Alnahdi, J. Niesen, A. M. Rucklidge

TL;DR
This paper investigates localized oscillatory patterns, called oscillons, in a PDE model with periodic forcing, focusing on non-zero wavenumber patterns and deriving amplitude equations that match experimental observations.
Contribution
It derives coupled forced complex Ginzburg-Landau equations from a PDE model with periodic forcing, revealing localized solutions and snaking behavior relevant to experiments.
Findings
Localized solutions exhibit snaking behavior.
Amplitude equations accurately predict oscillons near onset.
Model results align with experimental Faraday wave observations.
Abstract
In pattern-forming systems, localized patterns are readily found when stable patterns exist at the same parameter values as the stable unpatterned state. Oscillons are spatially localized, time-periodic structures, which have been found experimentally in systems that are driven by a time-periodic force, for example, in the Faraday wave experiment. This paper examines the existence of oscillatory localized states in a PDE model with single frequency time dependent forcing, introduced in [A. M. Rucklidge and M. Silber, SIAM J. Appl. Math., 8 (2009), pp. 298-347, arXiv:0805.0878] as a phenomenological model of the Faraday wave experiment. We choose parameters so that patterns set in with non-zero wavenumber (in contrast to [A. S. Alnahdi, J. Niesen and A. M. Rucklidge, SIAM J. Appl. Dyn. Syst., 13 (2014), pp. 1311-1327, arXiv:1312.2773]). In the limit of weak damping, weak detuning, weak…
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