Partial differential equations Definition
Turing pattern
Builds on Reaction–diffusion systemJacobian matrixEigenvalueLaplacian
Definition
Let , let be a diagonal matrix with positive diagonal entries, and let be smooth. Consider the reaction–diffusion system for , where is the Laplacian. Let satisfy and let be the Jacobian matrix of at . The uniform state is Turing unstable, or has a diffusion-driven instability, if:
- every eigenvalue of has negative real part, so is stable without diffusion;
- there is such that has an eigenvalue with positive real part.
A Turing pattern is a stationary, spatially non-constant solution near that bifurcates from a Turing unstable uniform state. It is typically periodic, with a wave number as in clause 2.
Remarks
The perturbation with a wave vector , , solves the linearised system exactly when is an eigenvalue of with eigenvector , which explains clause 2. Example: , , . Then and , so clause 1 holds. For , , so has a positive real eigenvalue and clause 2 holds. Non-example: if is a multiple of the identity, the eigenvalues of are those of shifted by , so clause 2 fails whenever clause 1 holds. For , a necessary condition is that the two diffusion coefficients differ.
Reading path
To understand this page from the ground up, read these 15 pages in order. The foundations come first.
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- no evidence level
- Eigenvalue concept
- Euclidean space object
- Function concept
- Reaction–diffusion system concept
- Total derivative concept
- Function of several variables concept
- Vector-valued function concept
- Differentiable function of several variables concept
- Partial derivative concept
- Vector field concept
- Gradient concept
- Jacobian matrix concept
- Divergence concept
- Laplacian concept
- Turing pattern definition
Further reading
About this page
| Tag | KSA55H8Q8N |
|---|---|
| URI | m2://KSA55H8Q8N |
| Kind | definition |
| Writing | W0 stub |
| MSC | 35B36, 35K57, 92C15 |
| Defines | Turing pattern |
| Uses | Reaction–diffusion system, Jacobian matrix, Eigenvalue, Laplacian |
| Changed | 2 November 2026 |
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