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Self-Organized Criticality

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Complex and Adaptive Dynamical Systems
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Abstract

Classically, a phase transition occurs when the properties of a system change upon tuning an external parameter, like the temperature. Is it possible, that a complex system regulates an internal parameter on its own, self-organized, such that it approaches a critical point all by itself? This is the central question discussed in this chapter.

Starting with an introduction to the Landau theory of phase transitions, particular attention will be devoted to cellular automata, an important and popular class of standardized dynamical systems. Cellular automata allow for an intuitive construction of models, such as the forest fire mode, the game of life, and the sandpile model, which exhibits “self-organized criticality”. Mathematically, a further understanding will be attained with the help of random branching theory. The chapter concludes with a discussion of whether self-organized criticality occurs in the most adaptive dynamical system of all, namely in the context of long-term evolution.

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Notes

  1. 1.

    Spontaneous symmetry breaking is not present for first-order transitions, at which properties change discontinuous, see Table 6.1.

  2. 2.

    From a dynamical systems point of view, the transition shown in Fig. 6.2 is equivalent to a pitchfork bifurcation, as detailed out Sect. 2.2.2 of Chap. 2.

  3. 3.

    The stability of the three solutions are treated in exercise (6.1).

  4. 4.

    Power laws in terms of scale-free degree distributions are a cornerstone of network theory, please consult Sect. 1.6 of Chap. 1.

  5. 5.

    A particularly important class of dynamical networks are studied in Chap. 7.

  6. 6.

    The concept of life at the edge of chaos was first develop in the context of information-processing networks, as discussed Chap. 7.

  7. 7.

    Generically, absorbing states are final configurations of Markov chains, as discussed in Sect. 3.3.2 of Chap. 3.

  8. 8.

    A fully self consistent mean-field theory of absorbing phase transitions in the presence of uncorrelated external driving is presented in Sect. 10.2.2 of Chap. 10.

  9. 9.

    An analogous situation occurs in the context of high-dimensional and/or random graphs, as discussed in Sect. 1.3.3 of Chap. 1, which are also loopless in the thermodynamic limit.

  10. 10.

    For an introduction to generating functions for probability distributions we refer to Sect. 1.3.2 of Chap. 1.

  11. 11.

    The evaluation of avalanche durations is the topic of exercise (6.8).

  12. 12.

    See Chap. 8.

  13. 13.

    The term “genotype” denotes the ensemble of genes. The actual form of an organism, the “phenotype”, is determined by the genotype plus environmental factors, like food supply during growth.

  14. 14.

    Stochastic escape is discussed in Sect. 3.5.2 of Chap. 3.

  15. 15.

    This procedure corresponds to a 2D Watts and Strogatz model, which is discussed in Sect. 1.5 of Chap. 1.

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Gros, C. (2024). Self-Organized Criticality. In: Complex and Adaptive Dynamical Systems. Springer, Cham. https://doi.org/10.1007/978-3-031-55076-8_6

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