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    Phase Transition in NK-Kauffman Networks and its Correction for Boolean Irreducibility

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    In a series of articles published in 1986 Derrida, and his colleagues studied two mean field treatments (the quenched and the annealed) for \textit{NK}-Kauffman Networks. Their main results lead to a phase transition curve Kc 2 pc(1βˆ’pc)=1 K_c \, 2 \, p_c \left( 1 - p_c \right) = 1 (0<pc<1 0 < p_c < 1 ) for the critical average connectivity Kc K_c in terms of the bias pc p_c of extracting a "11" for the output of the automata. Values of K K bigger than Kc K_c correspond to the so-called chaotic phase; while K<Kc K < K_c , to an ordered phase. In~[F. Zertuche, {\it On the robustness of NK-Kauffman networks against changes in their connections and Boolean functions}. J.~Math.~Phys. {\bf 50} (2009) 043513], a new classification for the Boolean functions, called {\it Boolean irreducibility} permitted the study of new phenomena of \textit{NK}-Kauffman Networks. In the present work we study, once again the mean field treatment for \textit{NK}-Kauffman Networks, correcting it for {\it Boolean irreducibility}. A shifted phase transition curve is found. In particular, for pc=1/2 p_c = 1 / 2 the predicted value Kc=2 K_c = 2 by Derrida {\it et al.} changes to Kc=2.62140224613… K_c = 2.62140224613 \dots We support our results with numerical simulations.Comment: 23 pages, 7 Figures on request. Published in Physica D: Nonlinear Phenomena: Vol.275 (2014) 35-4
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