2011
DOI: 10.1162/artl_a_00041
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Fisher Information at the Edge of Chaos in Random Boolean Networks

Abstract: We study the order-chaos phase transition in random Boolean networks (RBNs), which have been used as models of gene regulatory networks. In particular we seek to characterize the phase diagram in information-theoretic terms, focusing on the effect of the control parameters (activity level and connectivity). Fisher information, which measures how much system dynamics can reveal about the control parameters, offers a natural interpretation of the phase diagram in RBNs. We report that this measure is maximized ne… Show more

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Cited by 52 publications
(58 citation statements)
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References 26 publications
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“…This framework is called local information dynamics and has been successfully applied to unravel computation in swarms (Wang et al, 2011), in Boolean networks (Lizier et al, 2011b), and in neural models (Boedecker et al, 2012) and data (Wibral et al, 2014a) (also see Section 6 for details on these example applications).…”
Section: Analyzing Neural Coding and Goal Functions In A Domain-indepmentioning
confidence: 99%
“…This framework is called local information dynamics and has been successfully applied to unravel computation in swarms (Wang et al, 2011), in Boolean networks (Lizier et al, 2011b), and in neural models (Boedecker et al, 2012) and data (Wibral et al, 2014a) (also see Section 6 for details on these example applications).…”
Section: Analyzing Neural Coding and Goal Functions In A Domain-indepmentioning
confidence: 99%
“…Their results suggest that theoretically, we can predict critical thresholds in epidemics [14], which could be of a substantial value in health care. In practice, one of the challenges lies in pinpointing such critical thresholds in finite-size systems, where a precise identification of phase transitions requires an estimation of the rate of change of the order parameter, often from finite and/or distributed data [15,16].…”
Section: Introductionmentioning
confidence: 99%
“…We set J = 1 and k B = 2, for which T c ≈ 2.269 J k B ≈ 1.13 (the first analytical result on the phase transition in the 2D Ising model has been presented by Onsager [15]). The values of T span the range [1,2] at steps of 0.05. For each value of T, 10 runs are performed starting from random initial conditions chosen with −1 spin probability equal to 0.25, so as to start with an intermediate condition between µ = −1 and µ = 0 (we also ran experiments with different biases in the initial condition and did not observe any difference in the results).…”
Section: Results On the Ising Modelmentioning
confidence: 99%