Download Coexistence and Persistence of Strange Attractors by Antonio Pumarino, Angel J. Rodriguez PDF

By Antonio Pumarino, Angel J. Rodriguez

Even supposing chaotic behaviour had usually been saw numerically prior, the 1st mathematical evidence of the lifestyles, with optimistic chance (persistence) of odd attractors was once given through Benedicks and Carleson for the Henon family members, at the start of 1990's. Later, Mora and Viana tested unusual attractor can also be power in widespread one-parameter households of diffeomorphims on a floor which unfolds homoclinic tangency. This publication is ready the patience of any variety of unusual attractors in saddle-focus connections. The coexistence and endurance of any variety of unusual attractors in an easy third-dimensional situation are proved, in addition to the truth that infinitely a lot of them exist at the same time.

Show description

Read Online or Download Coexistence and Persistence of Strange Attractors PDF

Similar system theory books

Stochastic Differential Equations

This booklet offers an creation to the fundamental idea of stochastic calculus and its purposes. Examples are given through the textual content, so that it will encourage and illustrate the idea and express its value for plenty of purposes in e. g. economics, biology and physics. the fundamental proposal of the presentation is to begin from a few uncomplicated effects (without proofs) of the better situations and increase the idea from there, and to be aware of the proofs of the simpler case (which however are frequently sufficiently basic for plenty of reasons) so as to be capable to achieve quick the components of the idea that's most vital for the functions.

Algebraic Methods for Nonlinear Control Systems (Communications and Control Engineering)

This can be a self-contained creation to algebraic keep an eye on for nonlinear platforms compatible for researchers and graduate scholars. it's the first booklet facing the linear-algebraic method of nonlinear keep watch over platforms in any such specific and wide type. It presents a complementary method of the extra conventional differential geometry and offers extra simply with numerous very important features of nonlinear platforms.

Hyperbolic Chaos: A Physicist’s View

"Hyperbolic Chaos: A Physicist’s View” provides fresh development on uniformly hyperbolic attractors in dynamical structures from a actual instead of mathematical standpoint (e. g. the Plykin attractor, the Smale – Williams solenoid). The structurally good attractors occur robust stochastic homes, yet are insensitive to version of capabilities and parameters within the dynamical structures.

Fundamentals of complex networks : models, structures, and dynamics

Complicated networks equivalent to the web, WWW, transportation networks, energy grids, organic neural networks, and clinical cooperation networks of every kind offer demanding situations for destiny technological improvement. • the 1st systematic presentation of dynamical evolving networks, with many updated functions and homework initiatives to reinforce examine• The authors are all very lively and recognized within the speedily evolving box of complicated networks• complicated networks have gotten an more and more very important region of study• provided in a logical, positive sort, from simple via to complicated, interpreting algorithms, via to build networks and learn demanding situations of the longer term

Extra resources for Coexistence and Persistence of Strange Attractors

Sample text

Of course, s depends on w E P~. Given s C N and M E N , let ~Ts(M) be the number of all the components w~ for all w C P~, such t h a t Imll + ... + Im~l = M. Let 77(M) = E ~7,(M). 8) I- M . (,~,e,), with Imll + ... 9) CHAPTER 2. THE UNIMODAL FAMILY 50 it follows that m (XM) =~--~ rb(M)1~81 _< r/(M)Iwm,k[ exp ~ - ~ Irnl - M <_ s>0 _< I~,~,klexp - M + ~ Iml 9 Now, let us define Yu, t = XM N {a 9 (w,~,k) " Ei(a) = t}. (~,t = 0. 22, it follows that t = e i - ~ =~-~. ( v / + l - v i ) < 5- ~ i=0 ]rni[ = 5 ( M + [m[).

S we shall say t h a t #~ is a r e t u r n of co. F u r t h e r m o r e , if k < n - 1, then Rk(wk) = R~_l(w) n {m E N : m < k}. H . 3 . For each r e t u r n #i E P ~ - I there exists an associated interval I+,k~ with [rni[ > A, which is called the host interval of co at the return/,~, such t h a t ~,,(co,,) C I+,,k,. If CHAPTER 2. , #~ + p~} will be called the binding period associated to the return #i. For a suitable notation we write Po = - 1 . 4. , n - 1, wk satisfies (BAk) and (EGk). 13, it follows that Pi < ~+~ [mil.

18. Suppose that # < n is a return of co G P,~-I, with host interval I+,k. Let p be the length of its binding period and co, E P~ such that w C co,. 2) If it is an essential return and it' is the first return situation of w u after #, then I{,'(co~)l >- e~qe-~+~'m]. 2) If it is an essential return, and there exist no return situations of w , in the piece of orbit (it, n), then I{n(co)l >- e~q-~e-'~+~lml. Proof. (co)-----7- (x') (fp+1)' 1 (if),(x) e(I-~+~)I'~I. C H A P T E R 2. 1) follows by taking 6/3 < / 3 + c and a large enough A.

Download PDF sample

Rated 4.41 of 5 – based on 35 votes