Download e-book for kindle: Chaotic Dynamics and Transport in Classical and Quantum by P. Collet (auth.), P. Collet, M. Courbage, S. Métens, A.

By P. Collet (auth.), P. Collet, M. Courbage, S. Métens, A. Neishtadt, G. Zaslavsky (eds.)

ISBN-10: 1402029454

ISBN-13: 9781402029455

ISBN-10: 1402029462

ISBN-13: 9781402029462

ISBN-10: 1402029470

ISBN-13: 9781402029479

From the 18th to the thirtieth August 2003 , a NATO complicated examine Institute (ASI) used to be held in Cargèse, Corsica, France. Cargèse is a pleasant small village located by way of the mediterranean sea and the Institut d'Etudes Scientifiques de Cargese offers ? a standard position to arrange Theoretical Physics summer season faculties and Workshops * in a closed and good equiped position. The ASI was once a global summer season institution on "Chaotic Dynamics and shipping in Classical and Quantum Systems". the most objective of the college used to be to improve the mutual interplay among Physics and arithmetic pertaining to statistical houses of classical and quantum dynamical platforms. quite a few experimental and numerical observations have proven new phenomena of chaotic and anomalous delivery, fractal constructions, chaos in physics accelerators and in cooled atoms within atom-optics billiards, space-time chaos, fluctuations faraway from equilibrium, quantum decoherence and so forth. New theoretical equipment were constructed for you to modelize and to appreciate those phenomena (volume holding and ergodic dynamical structures, non-equilibrium statistical dynamics, fractional kinetics, coupled maps, space-time entropy, quantum dissipative approaches etc). the varsity collected a crew of experts from numerous horizons lecturing and discussing at the achievements, views and open difficulties (both basic and applied).

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Additional info for Chaotic Dynamics and Transport in Classical and Quantum Systems: Proceedings of the NATO Advanced Study Institute on International Summer School on Chaotic Dynamics and Transport in Classical and Quantum Systems Cargèse, Corsica 18–30 August 2003

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0 , ω1 , . ) in Ω the corresponding points of accumulation of islands should be different. Let P be a sticky riddle. For any ω = (i0 , i1 , . ,in−1 , define x = x(ω) := limn→∞ xn . The set Λ = {x(ω) : ω ∈ Ω} is said to be a sticky set. It is well defined thanks to Axioms (iii)–(v). , f |Λ has zero topological entropy. 3 Geometric constructions of sticky sets Some numerical observation [15] show that sometimes every island of stability Pi , together with all its satellites Pij , belongs to a basic set ∆i of a geometric construction.

2. Dynamical Chaos We give a definition of dynamical chaos following mainly Takens’ ideas see [39, 40] and [8]. Dynamical Chaos in Terms of the -complexity 41 We say that a signal (an observable) φ(t) is generated by a dynamical system (f t , M ) if there exist an initial point x0 belonging to M and the function ψ : M → R such that φ(t) = ψ(f t x0 ). Consider the case of discrete time t ∈ Z. Introduce space of all bounded observables b = {a = (a0 , a1 , . ), ai = φ(i) ∈ R} and endow it |ai | with the norm ||a|| = ∞ 0 2i , so that B becomes a Banach space.

In−1 , n > 0, then limn→∞ xn exists; (v) if xn ∈ Pi , yn ∈ Pj , |i| = |j| = n, n > 0, and i = j at least for one value of n then limn→∞ xn = limn→∞ yn . ,in−1 for any fixed ω = (i0 , . . , in−1 , . ); (v) for different points ω = (ω0 , ω1 , . ), ω = (ω0 , ω1 , . ) in Ω the corresponding points of accumulation of islands should be different. Let P be a sticky riddle. For any ω = (i0 , i1 , . ,in−1 , define x = x(ω) := limn→∞ xn . The set Λ = {x(ω) : ω ∈ Ω} is said to be a sticky set. It is well defined thanks to Axioms (iii)–(v).

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Chaotic Dynamics and Transport in Classical and Quantum Systems: Proceedings of the NATO Advanced Study Institute on International Summer School on Chaotic Dynamics and Transport in Classical and Quantum Systems Cargèse, Corsica 18–30 August 2003 by P. Collet (auth.), P. Collet, M. Courbage, S. Métens, A. Neishtadt, G. Zaslavsky (eds.)


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