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Existence boundary of Turing patterns at larger μ

Characterize the existence boundary of stationary wavetrains (Turing patterns) u(x) = u_p(kx) in the cubic Swift–Hohenberg equation ∂t u = −(1+Δ)^2 u + μ u − u^3 for non-small μ by determining the full bifurcation structure and delimiting curves in (k, μ)-parameter space, thereby fully describing the intricate existence boundary observed numerically.

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Background

Beyond the small-μ regime, the family of stationary wavetrains exhibits complex existence and bifurcation structures, with intricate boundaries in wavenumber–parameter space. The authors provide numerical evidence of such complexity, including at μ ≈ 0.9, prior to additional equilibria bifurcations.

They explicitly note that this existence boundary has not been fully explored, indicating the need for a comprehensive analysis and continuation of wavetrain solution branches and boundaries to map the full parameter space beyond weakly nonlinear predictions.

References

The intricate existence boundary of the Turing instability, shown in Figure~\ref{f:wt-existence} for \mu=0.9 (i.e. before the bifurcation of the additional equilibria), has yet to be fully explored as far as we are aware though there have been some investigations in this direction .