In pattern-forming systems, localized patterns are readily found when stablepatterns exist at the same parameter values as the stable unpatterned state.Oscillons are spatially localized, time-periodic structures, which have beenfound experimentally in systems that are driven by a time-periodic force, forexample, in the Faraday wave experiment. This paper examines the existence ofoscillatory localized states in a PDE model with single frequency timedependent 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 ofthe Faraday wave experiment. We choose parameters so that patterns set in withnon-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 forcing,small group velocity, and small amplitude, we reduce the model PDE to thecoupled forced complex Ginzburg-Landau equations. We find localized solutionsand snaking behaviour in the coupled forced complex Ginzburg-Landau equationsand relate these to oscillons that we find in the model PDE. Close to onset,the agreement is excellent. The periodic forcing for the PDE and the explicitderivation of the amplitude equations make our work relevant to theexperimentally observed oscillons.
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机译:在模式形成系统中,当稳定模式与稳定的未模式状态存在相同的参数值时,容易找到局部模式。振荡器是空间定位的时间周期结构,已在由时间周期力驱动的系统中通过实验找到,例如在法拉第波浪实验中。本文研究了单频时变强迫的PDE模型中的振荡局部状态的存在,[A。 [M. Rucklidge和M. Silber,SIAM J. Appl.Math。,8(2009),第298-347页,arXiv:0805.0878]作为法拉第波浪实验的现象学模型。我们选择参数以使模式设置为非零波数(与[AS Alnahdi,J.Niesen and AMRucklidge,SIAM J.Appl.Dyn.Syst。,13(2014),pp.1311-1327,arXiv: 1312.2773])。在弱阻尼,弱失谐,弱强迫,小群速度和小振幅的极限下,我们将模型PDE简化为耦合的强迫复数Ginzburg-Landau方程。我们在耦合的强迫复数Ginzburg-Landau方程中找到了局部解和蛇行行为,并将它们与我们在PDE模型中找到的振荡子相关联。即将发作,协议非常好。 PDE的周期性强迫和振幅方程的显式推导使我们的工作与实验观察到的振荡器有关。
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