The dynamics of disappearing pulses in a singularly perturbed reaction–diffusion system with parameters that vary in time and space

Abstract We consider the evolution of multi-pulse patterns in an extended Klausmeier equation with parameters that change in time and/or space. We formally show that the full PDE dynamics of a N -pulse configuration can be reduced to a N -dimensional dynamical system describing the dynamics on a N -dimensional manifold M N . Next, we determine the local stability of M N via the quasi-steady spectrum associated to evolving N -pulse patterns, which provides explicit information on the boundary ∂ M N . Following the dynamics on M N , a N -pulse pattern may move through ∂ M N and ‘fall off’ M N . A direct nonlinear extrapolation of our linear analysis predicts the subsequent fast PDE dynamics as the pattern ‘jumps’ to another invariant manifold M M , and specifically predicts the number N − M of pulses that disappear. Combining the asymptotic analysis with numerical simulations of the dynamics on the various invariant manifolds yields a hybrid asymptotic–numerical method describing the full process that starts with a N -pulse pattern and typically ends in the trivial homogeneous state without pulses. We extensively test this method against PDE simulations and deduce general conjectures on the nature of pulse interactions with disappearing pulses. We especially consider the differences between the evolution of irregular and regular patterns. In the former case, the disappearing process is gradual: irregular patterns lose their pulses one by one. In contrast, regular, spatially periodic, patterns undergo catastrophic transitions in which either half or all pulses disappear. However, making a precise distinction between these two drastically different processes is quite subtle, since irregular N -pulse patterns that do not cross ∂ M N typically evolve towards regularity. hybrid asymptotic-numerical method

[1]  Keith Promislow,et al.  A Renormalization Method for Modulational Stability of Quasi-Steady Patterns in Dispersive Systems , 2002, SIAM J. Math. Anal..

[2]  Jens D. M. Rademacher First and Second Order Semistrong Interaction in Reaction-Diffusion Systems , 2013, SIAM J. Appl. Dyn. Syst..

[3]  J. Sherratt History-dependent patterns of whole ecosystems , 2013 .

[4]  Arjen Doelman,et al.  Slowly Modulated Two-Pulse Solutions in the Gray--Scott Model II: Geometric Theory, Bifurcations, and Splitting Dynamics , 2001, SIAM J. Appl. Math..

[5]  Michael J. Ward,et al.  Oscillatory instabilities and dynamics of multi-spike patterns for the one-dimensional Gray-Scott model , 2009, European Journal of Applied Mathematics.

[6]  Geertje Hek,et al.  Rise and Fall of Periodic Patterns for a Generalized Klausmeier–Gray–Scott Model , 2013, J. Nonlinear Sci..

[7]  Keith Promislow,et al.  Adiabatic stability under semi-strong interactions: The weakly damped regime , 2013, 1301.4466.

[8]  E. Meron,et al.  Gradual regime shifts in spatially extended ecosystems , 2012, Theoretical Ecology.

[9]  Arjen Doelman,et al.  Spectra and Stability of Spatially Periodic Pulse Patterns: Evans Function Factorization via Riccati Transformation , 2015, SIAM J. Math. Anal..

[10]  David Dunkerley,et al.  Vegetation Mosaics of Arid Western New South Wales, Australia: Considerations of Their Origin and Persistence , 2014 .

[11]  C. Klausmeier,et al.  Regular and irregular patterns in semiarid vegetation , 1999, Science.

[12]  J. Tzou,et al.  Slowly varying control parameters, delayed bifurcations, and the stability of spikes in reaction-diffusion systems , 2014, 1401.5359.

[13]  J. Bogaert,et al.  Determinants and dynamics of banded vegetation pattern migration in arid climates , 2012 .

[14]  Juncheng Wei,et al.  The existence and stability of spike equilibria in the one-dimensional Gray-Scott model on a finite domain , 2005, Appl. Math. Lett..

[15]  E. Meron Nonlinear Physics of Ecosystems , 2015 .

[16]  Robert Gardner,et al.  Stability analysis of singular patterns in the 1-D Gray-Scott model I: a matched asymptotics approach , 1998 .

[17]  Michael J. Ward,et al.  The Dynamics of Multispike Solutions to the One-Dimensional Gierer--Meinhardt Model , 2002, SIAM J. Appl. Math..

[18]  Derin B. Wysham,et al.  Regime shifts in ecological systems can occur with no warning. , 2010, Ecology letters.

[19]  Arnd Scheel,et al.  Instabilities of Wave Trains and Turing Patterns in Large Domains , 2007, Int. J. Bifurc. Chaos.

[20]  E. Meron,et al.  Ecosystem engineers: from pattern formation to habitat creation. , 2004, Physical review letters.

[21]  M. Rietkerk,et al.  Self-Organized Patchiness and Catastrophic Shifts in Ecosystems , 2004, Science.

[22]  J. E. Pearson Complex Patterns in a Simple System , 1993, Science.

[23]  Frits Veerman,et al.  Breathing pulses in singularly perturbed reaction-diffusion systems , 2015 .

[24]  W. Chen,et al.  The Stability and Dynamics of Localized Spot Patterns in the Two-Dimensional Gray-Scott Model , 2010, SIAM J. Appl. Dyn. Syst..

[25]  Frits Veerman,et al.  Pulses in a Gierer-Meinhardt Equation with a Slow Nonlinearity , 2013, SIAM J. Appl. Dyn. Syst..

[26]  Maarten B. Eppinga,et al.  Beyond Turing: The response of patterned ecosystems to environmental change , 2014 .

[27]  Frits Veerman,et al.  Destabilization Mechanisms of Periodic Pulse Patterns Near a Homoclinic Limit , 2018, SIAM J. Appl. Dyn. Syst..

[28]  Johan van de Koppel,et al.  Regular pattern formation in real ecosystems. , 2008, Trends in ecology & evolution.

[29]  Arjen Doelman,et al.  Spatially Periodic Multipulse Patterns in a Generalized Klausmeier-Gray-Scott Model , 2017, SIAM J. Appl. Dyn. Syst..

[30]  Arjen Doelman,et al.  Semistrong Pulse Interactions in a Class of Coupled Reaction-Diffusion Equations , 2003, SIAM J. Appl. Dyn. Syst..

[31]  Arjen Doelman,et al.  Homoclinic Stripe Patterns , 2002, SIAM J. Appl. Dyn. Syst..

[32]  Keith Promislow,et al.  Nonlinear Asymptotic Stability of the Semistrong Pulse Dynamics in a Regularized Gierer-Meinhardt Model , 2007, SIAM J. Math. Anal..

[33]  A. Doelman,et al.  Striped pattern selection by advective reaction-diffusion systems: resilience of banded vegetation on slopes. , 2015, Chaos.

[34]  Jonathan A. Sherratt,et al.  Using wavelength and slope to infer the historical origin of semiarid vegetation bands , 2015, Proceedings of the National Academy of Sciences.

[35]  M. Ward,et al.  Pulse‐Splitting for Some Reaction‐Diffusion Systems in One‐Space Dimension , 2005 .

[36]  Arjen Doelman,et al.  Slowly Modulated Two-Pulse Solutions in the Gray--Scott Model I: Asymptotic Construction and Stability , 2000, SIAM J. Appl. Math..

[37]  Michael J. Ward,et al.  The existence and stability of spike equilibria in the one-dimensional Gray-Scott model: the pulse-splitting regime , 2005 .

[38]  Robert Gardner,et al.  Large stable pulse solutions in reaction-diffusion equations , 2001 .

[39]  P. B. Mitchell,et al.  Vegetation arcs and litter dams: Similarities and differences , 1999 .

[40]  J. Tzou,et al.  Patterned vegetation, tipping points, and the rate of climate change , 2015, European Journal of Applied Mathematics.

[41]  Björn de Rijk,et al.  Spectra and Stability of Spatially Periodic Pulse Patterns II: The Critical Spectral Curve , 2018, SIAM J. Math. Anal..

[42]  Keith Promislow,et al.  Front Interactions in a Three-Component System , 2010, SIAM J. Appl. Dyn. Syst..

[43]  Wentao Sun,et al.  The Slow Dynamics of Two-Spike Solutions for the Gray-Scott and Gierer-Meinhardt Systems: Competition and Oscillatory Instabilities , 2005, SIAM J. Appl. Dyn. Syst..

[44]  Arjen Doelman,et al.  Hopf dances near the tips of Busse balloons , 2011 .

[45]  Wei-Ming Ni,et al.  DIFFUSION, CROSS-DIFFUSION, AND THEIR SPIKE-LAYER STEADY STATES , 1998 .

[46]  Michael J. Ward,et al.  Slow translational instabilities of spike patterns in the one-dimensional Gray-Scott model , 2006 .

[47]  Michael J. Ward,et al.  Transition to blow-up in a reaction–diffusion model with localized spike solutions† , 2017, European Journal of Applied Mathematics.