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he expected hitting time using combinatorial analysis (see Text SI for details). We now present the basic intuitive arguments of the main results. Markov chain on the one-dimensional grid For a single broad peak, due to symmetry we can interpret the evolutionary random walk as a Markov chain on the o
logy I www.ploscompbiol.org 3 September 2014 I Volume 10 I Issue 9 I el 0038113 EFTA00611790 The Time Scale of Evolutionary Innovation Table 1. Numerical data for discovery time in flat fitness landscapes. r.i 3 1 2 3 r= - 4 L=103 1.021011 136.107 183 L=101 3.8910I” 1.28.104' 2666 Numerical
s another interesting problem. Materials and Methods Our results are based on a mathematical analysis of the underlying stochastic processes. For Markov chains on the one- dimensional grid, we describe recurrence relations for the expected hitting time and present lower and upper hounds on the expec
iology I www.ploscompbiol.org 3 September 2014 I Volume 10 I Issue 9 I e1003818 EFTA00611783 The Time Scale of Evolutionary Innovation Table 1. Numerical data for discovery time in flat fitness landscapes. r.I L=102 1.021018 7.36107 183 L=10' 5.89 1.28.100 2666 Numerical data for the discover
d in discrete conductance events with a small set of characteristic open and closed times. The distributions of each of could be fitted with its own, Markov process derived, exponential. With technical advances and improved temporal resolution, more characteristic times and their associated a = 2 exponent
nt and attractor dimension curves of EEG in sleep. Comput Biol Med 26:419-428 Press, W.H., Flannery, B.P., Teukolsky, S.A., Vetterling, W.T. (1991) Numerical Recipies; The Art of Scientific Computing. Cambridge University Press, Cambridge. Pritchard, W.S. (1992) The brain in fractal time: 1/f-like power s
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