Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden Modes

We study the emergence of strong interactions between dissipative coherent structures (pulses) in spatially extended systems. Focusing first on a prototypical model problem from fluid dynamics, that of liquid film flowing down a vertical plane, we show that under certain conditions, a two-pulse syst...

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Main Authors: Alex Round, Te-Sheng Lin, Marc Pradas, Dmitri Tseluiko, Serafim Kalliadasis
Format: Article
Language:English
Published: American Physical Society 2025-07-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.15.031010
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author Alex Round
Te-Sheng Lin
Marc Pradas
Dmitri Tseluiko
Serafim Kalliadasis
author_facet Alex Round
Te-Sheng Lin
Marc Pradas
Dmitri Tseluiko
Serafim Kalliadasis
author_sort Alex Round
collection DOAJ
description We study the emergence of strong interactions between dissipative coherent structures (pulses) in spatially extended systems. Focusing first on a prototypical model problem from fluid dynamics, that of liquid film flowing down a vertical plane, we show that under certain conditions, a two-pulse system undergoes a transition from a regime of decaying oscillatory dynamics to one with self-sustained oscillations. Intriguingly, such a transition is not governed by the standard Hopf bifurcation. Instead, a novel governing mechanism for transition to oscillatory dynamics is unraveled via a peculiar and atypical Hopf bifurcation in which a complex-conjugate resonance pair crosses the imaginary axis in the complex plane. Prior to crossing the essential spectrum (including at the bifurcation point), this resonance pair does not appear in the standard L_{C}^{2}-based spectral analysis but reveals itself when appropriate weighted functional spaces are used. We show that such a resonance pair originates from the splitting of a resonance pole of the single-pulse system. While this object is not part of the classical spectrum, it plays a vital role in shaping the system’s dynamics. We further demonstrate that this resonance-pole mechanism extends to a broad range of systems. Specifically, in the generalised Kuramoto-Sivashinsky equation—a model prototype applicable across a wide range of fields from fluid dynamics to geophysics and plasma physics—we observe the same bifurcation and resulting oscillatory pulse interactions. By contrast, in the FitzHugh-Nagumo model—a central model prototype in reaction-diffusion systems—the resonance pole splits into real eigenvalues, and monotonic pulse interactions occur. In addition, we illustrate that the resonance pole may induce oscillatory interactions in three-pulse systems and eventually lead to chaotic dynamics in strongly interacting multipulse systems, which can be quantified in terms of a positive Lyapunov exponent.
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spelling doaj-art-f19d12f6f0d04bdc84e331a9a173b6d12025-07-09T17:05:34ZengAmerican Physical SocietyPhysical Review X2160-33082025-07-0115303101010.1103/PhysRevX.15.031010Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden ModesAlex RoundTe-Sheng LinMarc PradasDmitri TseluikoSerafim KalliadasisWe study the emergence of strong interactions between dissipative coherent structures (pulses) in spatially extended systems. Focusing first on a prototypical model problem from fluid dynamics, that of liquid film flowing down a vertical plane, we show that under certain conditions, a two-pulse system undergoes a transition from a regime of decaying oscillatory dynamics to one with self-sustained oscillations. Intriguingly, such a transition is not governed by the standard Hopf bifurcation. Instead, a novel governing mechanism for transition to oscillatory dynamics is unraveled via a peculiar and atypical Hopf bifurcation in which a complex-conjugate resonance pair crosses the imaginary axis in the complex plane. Prior to crossing the essential spectrum (including at the bifurcation point), this resonance pair does not appear in the standard L_{C}^{2}-based spectral analysis but reveals itself when appropriate weighted functional spaces are used. We show that such a resonance pair originates from the splitting of a resonance pole of the single-pulse system. While this object is not part of the classical spectrum, it plays a vital role in shaping the system’s dynamics. We further demonstrate that this resonance-pole mechanism extends to a broad range of systems. Specifically, in the generalised Kuramoto-Sivashinsky equation—a model prototype applicable across a wide range of fields from fluid dynamics to geophysics and plasma physics—we observe the same bifurcation and resulting oscillatory pulse interactions. By contrast, in the FitzHugh-Nagumo model—a central model prototype in reaction-diffusion systems—the resonance pole splits into real eigenvalues, and monotonic pulse interactions occur. In addition, we illustrate that the resonance pole may induce oscillatory interactions in three-pulse systems and eventually lead to chaotic dynamics in strongly interacting multipulse systems, which can be quantified in terms of a positive Lyapunov exponent.http://doi.org/10.1103/PhysRevX.15.031010
spellingShingle Alex Round
Te-Sheng Lin
Marc Pradas
Dmitri Tseluiko
Serafim Kalliadasis
Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden Modes
Physical Review X
title Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden Modes
title_full Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden Modes
title_fullStr Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden Modes
title_full_unstemmed Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden Modes
title_short Coherent Structure Interactions in Spatially Extended Systems Driven by Excited Hidden Modes
title_sort coherent structure interactions in spatially extended systems driven by excited hidden modes
url http://doi.org/10.1103/PhysRevX.15.031010
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AT serafimkalliadasis coherentstructureinteractionsinspatiallyextendedsystemsdrivenbyexcitedhiddenmodes