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Self Organization

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Complex and Adaptive Dynamical Systems
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Abstract

Self-organized pattern formation occurs when complex spatio-temporal structures result from seemingly simple dynamical evolution processes. The formation of animal markings can be understood in this context in terms of a Turing instability. Zebra stripes, and other biological patterns, emerge in reaction-diffusion systems, which will be discussed together with the notion of self-stabilizing wavefronts, as observed for the Fisher equation.

Further prominent examples of self-organizing processes treated in this chapter involve collective decision making and swarm intelligence, as occurring in social insects and flocking birds, information offloading in terms of stigmergy, opinion dynamics and the physics of traffic flows, including the ubiquitous phenomenon of self-organized traffic congestions.

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Notes

  1. 1.

    Diffussion is treated in depth in Sect. 3.3 of Chap. 3.

  2. 2.

    The entries of Jacobian matrix are the derivatives of the flow, see Sect. 2.2 of Chap. 2.

  3. 3.

    Diffusion Green’s functions are introduced in Sect. 3.3 of Chap. 3.

  4. 4.

    Recall the expression \(\mathrm {i}\hbar \frac {\partial \psi }{\partial t} = - \frac {\hbar ^2}{2m}\varDelta \psi + V \psi \) for the time-dependent one dimensional Schrödinger equation. Equation (4.23) is recovered for an exponential time dependency \(\sim \!\exp (-i\lambda t/\hbar )\) of the wavefunction \(\psi \).

  5. 5.

    For the Van der Pol oscillator, secular perturbation theory is developed in Sect. 3.2 of Chap. 3.

  6. 6.

    As a reminder, note that a node/focus has real/complex Lypunov exponents, as defined in Sect. 2.2 of Chap. 2.

  7. 7.

    Bifurcation theory is discussed in Sect. 2.2.2 of Chap. 2.

  8. 8.

    A prototypical example are the boolean networks discussed in Chap. 7.

  9. 9.

    The generic framework for phase transitions,, the Ginzburg-Landau theory, is developed in Sect. 6.1 of Chap. 6.

  10. 10.

    An analogous rescaling is done when deriving the diffusion equation \(\dot p = D\varDelta p\),as discussed in Sect. 3.3.1 of Chap. 3.

  11. 11.

    The classical voter model is treated in exercise (4.8).

  12. 12.

    The general theory of dynamical systems with time delays is developed in Sect. 2.5 of Chap. 2.

  13. 13.

    This result is in accordance with our discussion in Sect. 2.5 of Chap. 2, regarding the influence of time delays in ordinary differential equations.

References

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Gros, C. (2024). Self Organization. In: Complex and Adaptive Dynamical Systems. Springer, Cham. https://doi.org/10.1007/978-3-031-55076-8_4

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