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9), grouping together the terms of the same total symbol string length ☞ sect. 3 1/ζ = (1 − t0 )(1 − t1 )(1 − t10 )(1 − t100 ) · · · = 1 − t0 − t1 − [t10 − t1 t0 ] − [(t100 − t10 t0 ) + (t101 − t10 t1 )] −[(t1000 − t0 t100 ) + (t1110 − t1 t110 ) +(t1001 − t1 t001 − t101 t0 + t10 t0 t1 )] − . . 10) The virtue of the expansion is that the sum of all terms of the same total length n (grouped in brackets above) is a number that is exponentially smaller than a typical term in the sum, for geometrical reasons we explain in the next section.

16]. In Ruelle’s monograph transfer operator technique (or the “Perron-Frobenius theory”) and Smale’s theory of hyperbolic flows are applied to zeta functions and correlation functions. 17]. 20]. 4] covers the same ground in more depth. 22] offers a nice introduction to the problem of irreversibility in dynamics. 23]. ”, the answer is yes indeed, there is a line of research in study on neuronal dynamics that focuses on possible unstable periodic states, described for example in ref. 25]. Guide to exercises God can afford to make mistakes.

An introductory course should give students skills in qualitative and numerical analysis of dynamical systems for short times (trajectories, fixed points, bifurcations) and familiarize them with Cantor sets and symbolic dynamics for chaotic dynamics. With this, and a graduate level exposure to statistical mechanics, partial differential equations and quantum mechanics, the stage is set for any of the one-semester advanced courses based on this book. The courses taught so far start out with the introductory chapters on qualitative dynamics, symbolic dynamics and flows, and then continue in different directions: Deterministic chaos.

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Classical & Quantum Chaos by Predrag Cvitanovic' et alpdftitle


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