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.
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 .
                — Numerical Continuation and Bifurcation in Nonlinear PDEs: Stability, invasion and wavetrains in the Swift-Hohenberg equation
                
                (2502.03858 - Lloyd et al., 6 Feb 2025) in Section 6 (Discussion)