Abstract
We discuss some aspects of the asymptotic behavior of the forward orbits of most points for piecewise smooth maps of the interval, specially for contracting Lorenz maps. We are particularly interested in the statistical aspects of most orbits, the existence of statistical attractors and how most orbits in the basin of attraction of an attracting Cantor sets approach the attractor.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
References
V.S. Afraimovich, V.V. Bykov, L.P. Shil’nikov, On the appearance and structure of the Lorenz attractor. Dokl. Acad. Sci. USSR 234, 336–339 (1977)
J.F. Alves, M. Soufi, Statistical stability and limit laws for Rovella maps. Nonlinearity 25(12), 3527–3552 (2012)
A. Arneodo, P. Coullet, C. Tresser, A possible new mechanism for the onset of turbulence. Phys. Lett. A 81(4), 197–201 (1981)
V.I. Arnold, V.S. Afrajmovich, Y. Ilyashenko, L.P. Shilnikov, Bifurcation Theory and Catastrophe Theory (Springer-Verlag, Berlin, Heidelberg, 1999)
V. Araujo, A. Castro, M.J. Pacifico, V. Pinheiro, Multidimensional Rovella-like attractors. J. Differ. Equations 3163–3201 (2011)
L. Alsedà , J. Llibre, M. Misiurewicz, C. Tresser, Periods and entropy for Lorenz-like maps. Ann. Inst. Fourier 39, 929–952 (1989)
A. Blokh, M. Lyubich, Measurable dynamics of \(S\)-unimodal maps of the interval. Ann. Sci. École Norm. Sup. 24, 545–573 (1991)
P. Brandão, On the structure of contracting Lorenz maps, to appear on Annales de l’Institut Henri Poincaré. Analyse Non Linéaire (2018). https://doi.org/10.1016/j.anihpc.2017.12.001
P. Brandão, J. Palis, V. Pinheiro, On the finiteness of attractors for one-dimensional maps with discontinuities (2013). arXiv:1401.0232
P. Brandão, J. Palis, V. Pinheiro, On the finiteness of attractors for piecewise C\(^2\) maps of the interval. Erg. Theo. Dyn. Sys. 261, 1–21 (2017)
H. Bruin, G. Keller, T. Nowicki, S.J. van Strien, Wild Cantor attractors exist. Ann. Math. 143, 97–130 (1996)
E. Catsigeras, On Ilyashenko’s statistical attractors. CDSS. 29, 78–97 (2013)
T. Cherry, Analytic quasi-periodic curves of discontinuous type on the torus. Proc. London Math. Soc. 44, 175–215 (1938)
P. Collet, P. Coullet, C. Tresser, Scenarios under constraint. J. Phyique Lett. 46, 143–147 (1985)
A. Denjoy, Sur les courbes definies par les équations différentielles à la surface du tore. J. de Mathématiques Pures et Appliquées 11, 333–375 (1930)
J.M. Gambaudo, C. Tresser, Dynamique réguliére ou chaotique. Applications du cercle ou de l’intervalle ayant une discontinuité. Comptes Rendus Acad. Sci. Paris, Ser I. 300, 311–313 (1985)
J. Guckenheimer, R.F. Williams, Structural stability of Lorenz attractors. Publ. Math. IHES 50, 59–72 (1979)
F. Hofbauer, G. Keller, Quadratic maps without asymptotic measure. Commun. Math. Phys. 127, 319–337 (1990)
G. Keller, M.S. Pierre, Topological and measurable dynamics of Lorenz maps, in Ergodic Theory, Analysis, and Efficient Simulation of Dynamical Systems, ed. by B. Fiedler (Springer, Berlin, Heidelberg, 2001)
R. Labarca, C.G. Moreira, Essential dynamics for Lorenz maps on the real line and the lexicographical world. Annales de l’Institut Henri Poincaré. Analyse Non Linéaire 23, 683694 (2006)
M. Lyubich, Non-existence of wandering intervals and structure of topological attractors of one dimensional dynamical systems: Schwarzian derivative. Ergod. Theory Dyn. Syst. 9, 737–749 (1989)
R. Mañé, R. Mane, Hyperbolicity, sinks and measure in one dimensional dynamics. Commun. Math. Phys. 100(4), 495–524, Commun. Math. Phys. (1987) 112, 721–724 (Erratum) (1985)
M. Martens, P. Mendes, W. de Melo, S. van Strien, On Cherry flows. Ergod. Theory Dyn. Syst. 10, 531–554 (1990)
M. Martens, W. de Melo, Universal models for Lorenz maps (pre-print version, 1996), de Melo’s homepage at IMPA. http://w3.impa.br/%7Edemelo/lorenz.ps
M. Martens, W. de Melo, Universal models for Lorenz maps. Ergod. Theory Dyn. Syst. 21, 833–860 (2001)
R. Metzger, Sinai-Ruelle-Bowen measures for contracting Lorenz maps and flows (Annales de l’Institut Henri Poincaré, Analyse Non Linéaire, 2000)
W. de Melo, S. van Strien, A structure theorem in one dimensional dynamics. Ann. Math. 129, 519–546 (1989)
W.C. de Melo, S.V. Strien, One Dimensional Dynamics (Springer 1993)
B. Mestel, D. Berry, Wandering intervals for Lorenz maps with bounded nonlinearity. Bull. Lond. Math. 23, 183–189 (1991)
J. Milnor, On the concept of attractor. Commun. Math. Phys. 99, 177–195 (1985)
M.J. Pacifico, M.J. Todd, Thermodynamic formalism for contracting Lorenz flows. Stat. Phys. 139(1), 159–176 (2010)
M. St. Pierre, Topological and measurable dynamics of Lorenz maps. Dissertationes Mathematicae,17 (1999)
I. Procaccia, S. Thomas, C. Tresser, Frist-return maps as a unifield renormalization scheme for dynamical systems. Phys. Rev. A. 35, 1–17 (1986)
A. Rovella, The dynamics of perturbations of contracting Lorenz maps. Bul. Soc. Brazil Mat. (N.S.) 24(2), 233–259 (1993)
C. Tresser, Nouveaux types de transitions vers une entropie topologique positive. Comptes Rendus Acad. Sci. Paris, Ser I. 296, 729–732 (1983)
C. Tresser, R.F. Williams, Splitting words and Lorenz braids. Phys. D 62, 15–21 (1993)
W. Tucker, The Lorenz attractor exists. C. R. Acad. Sci. Paris, Série I 328, 1197–1202 (1999)
S. van Strien, E. Vargas, Real bounds, ergodicity and negative Schwarzian for multimodal maps. J. Am. Math. Soc. 17, 749–782 (2004)
Author information
Authors and Affiliations
Corresponding author
Editor information
Editors and Affiliations
Appendix
Appendix
A homterval is an open interval \(I=(a,b)\) such that \(f^n|_I\) is a homeomorphism for \(n\ge 1\). This is equivalent to assume that \(I\cap \mathcal {O}_f^-(\mathcal {C}_f)=\emptyset \). A homterval I is called a wandering interval if \(I\cap {\mathbb B}_0(f)=\emptyset \) and \(f^j(I)\cap f^k(I)=\emptyset \) for all \(1\le j<k\), where \({\mathbb B}_0(f)\) the union of the basins of attraction of all periodic-like attractors.
Lemma 3.9
(Homterval Lemma, see [28]) Let \(I=(a,b)\) be a homterval of f. If I is not a wandering interval, then \(I\subset {\mathbb B}_0(f)\cup \mathcal {O}_f^{-}({\text {Per}}(f))\). Furthermore, if f is \(C^3\) with \(Sf<0\), and I is not a wandering interval, then the set \(I\setminus {\mathbb B}_0\) has at most one point.
Lemma 3.10
(Koebe’s Lemma [28]) For every \(\varepsilon >0\), \(\exists K>0\) such that the following holds: Let M, T be intervals in \({\mathbb R}\) with \(M\subset T\) and denote respectively by L and R the left and right components of \(T\setminus M\). If \(f:T\rightarrow f(T)\subset {\mathbb R}\) is a \(C^3\) diffeomorphism with negative Schwarzian derivative and
then \(\frac{|Df(x)|}{|Df(y)|}\le K\) for \(x,y\in M\).
Proposition 3.11
[See Proposition 3 in [10] and Proposition 2 of [38]] Let \(\mathcal {C}_f\subset (0,1)\) be a finite set. If \(f:[0,1]\setminus \mathcal {C}_f\rightarrow [0,1]\) is a \(C^2\) non-flat local diffeomorphism, then there exists a function \(O(\varepsilon )\) with \(O(\varepsilon )\rightarrow 0\) as \(\varepsilon \searrow 0\) with the following property: Let \(J\subset T\) be an interval, R, L the connected components of \(T\setminus J\) and \(\delta :=\min \{|R|/|J|,|L|/|J|\}\). Let n be an integer and \(T_0 \supset J_0\) intervals such that \(f^n|_{T_0}\) is a diffeomorphism, \(f^n(T_0)=T\) and \(f^n(J_0)=J\). If \(\varepsilon :=\max \{|f^j(T_0)|\,;\,0\le j\le n\}\), then
-
(1)
\( \big |\frac{Df^n(x)}{Df^n(y)}\big |\le \big (\frac{1+\delta }{\delta }\big )^2 e^{O(\varepsilon )\sum _{i=0}^{n-1}|f^i(J_0)|}\), for all \(x,y\in J_0\);
-
(2)
\(\exists \delta '>0\) depending only on \(\varepsilon \) and \(\sum _{i=0}^{n-1}|f^i(J_0)|\) such that, for all \(x,y\in J_0\) and \(1\le j\le n\), we have \( \big |\frac{Df^j(x)}{Df^j(y)}\big |\le \big (\frac{1+\delta '}{\delta '}\big )^2 e^{O(\varepsilon )\sum _{i=0}^{n-1}|f^i(J_0)|}\);
-
(3)
\(\frac{|Df^n(x)|}{|Df^n(y)|}\le \exp \big (\frac{2}{\delta |J|}|f^n(x)-f^n(y)|+O(\varepsilon )\sum _{i=0}^{n-1}|f^i(x)-f^j(y)|\big )\) for every \(x,y\in J_0\).
Proposition 3.12
(Proposition 3.4 for maps with negative Schwarzian derivative) Let U be an open subset of an interval (a, b) and \(F:U\rightarrow (a,b)\) be a \(C^3\) local diffeomorphism with negative Schwarzian derivative and such that \(F(P)=(a,b)\) for every connected component of U. If \({\mathbb B}(F)\) denotes the union of all wandering intervals of F with the basin of attraction of all periodic-like attractors of F, then
Furthermore, if \({\text {Leb}}\big (\bigcap _{n\ge 0}F^{-n}((a,b))\setminus {\mathbb B}(F)\big )=b-a\) then \({\text {Leb}}|_{(a,b)}\) is F strongly ergodic and \(\omega _F(x)=[a,b]\) for almost every \(x\in (a,b)\).   \(\square \)
Proof
Similar to the proof of Proposition 3.4. Essentially, one only need to replace Proposition 3.11 by Koebe’s Lemma (Lemma 3.10).
Proof of Proposition 2.5 As the attractor A is a cycle of intervals, we get from Theorem 1 that \(\omega _f(x)=A\) for almost every \(x\in [0,1]\). In particular, this forbids f to have wandering intervals and periodic attractors. As \(\overline{\mathcal {O}_f^+(c_-)\cup \mathcal {O}_f^+(c_+)}\) has empty interior, we can consider a connected component \(J\ne \emptyset \) of \(A\setminus ( \overline{\mathcal {O}_f^+(c_-)\cup \mathcal {O}_f^+(c_+)})\). As \(\overline{\mathcal {O}_f^+(c_-)\cup \mathcal {O}_f^+(c_+)}\ne A\), A is not a minimal set and so it cannot be a Cherry attractor. Hence, it follows from Theorem D of [8] that A is a chaotic cycle of intervals. In particular, this implies that \(\overline{{\text {Per}}(f)\cap A}=A\). Thus, choose \( q,p\in {\text {Per}}(f)\cap {\text {interior}}(J)\) with \(p<q\). Let I be any connected component of \((p,q)\setminus \overline{\mathcal {O}_f^+(c_-)\cup \mathcal {O}_f^+(c_+)}\). Note that I is a nice interval, that is, \(\mathcal {O}_f^+(\partial I)\cap I=\emptyset \). Let \(I^*=\{x\in \ I\,;\,\mathcal {O}_f^+(f(x))\cap I\ne \emptyset \}\) and \(F:I^*\rightarrow I\) the first return map, by f, to I. As \(\omega _f(x)\supset I\) for almost every \(x\in [0,1]\) and \({\text {Leb}}\circ f^{-1}\ll {\text {Leb}}\), we get that \({\text {Leb}}(I)={\text {Leb}}(I^*)={\text {Leb}}(\bigcap _{n\ge 0}F^{-1}(I^*))\). Thus, it follows from Proposition 3.12 that \({\text {Leb}}|_I\) is strongly ergodic with respect to F, in particular, F is ergodic.
The ergodicity of \({\text {Leb}}|_I\) with respect to f implies that \({\text {Leb}}\) is also ergodic with respect to f. Indeed, if \(V=f^{-1}(V)\) and \({\text {Leb}}(V)>0\) then, as \({\text {Leb}}\circ f^{-1}\ll {\text {Leb}}\) and \(\mathcal {O}_f^+(x)\cap I\ne \emptyset \) for \({\text {Leb}}\) almost all \(x\in [0,1]\), we get that \({\text {Leb}}(V\cap I)>0\). As F is the first return map to I, it follows that \(F^{-1}(V\cap I)=V\cap I\). Thus, by the ergodicity with respect to F, \({\text {Leb}}(V\cap I)={\text {Leb}}(I)\). That is, \({\text {Leb}}(I\setminus V)=0\). Using that \({\text {Leb}}\circ f^{-1}\ll {\text {Leb}}\), we get that \({\text {Leb}}([0,1]\setminus V)=0\), proving that \({\text {Leb}}\) is ergodic with respect to f.
Rights and permissions
Copyright information
© 2019 Springer Nature Switzerland AG
About this paper
Cite this paper
Brandão, P., Palis, J., Pinheiro, V. (2019). On the Statistical Attractors and Attracting Cantor Sets for Piecewise Smooth Maps. In: Pacifico, M., Guarino, P. (eds) New Trends in One-Dimensional Dynamics. Springer Proceedings in Mathematics & Statistics, vol 285. Springer, Cham. https://doi.org/10.1007/978-3-030-16833-9_4
Download citation
DOI: https://doi.org/10.1007/978-3-030-16833-9_4
Published:
Publisher Name: Springer, Cham
Print ISBN: 978-3-030-16832-2
Online ISBN: 978-3-030-16833-9
eBook Packages: Mathematics and StatisticsMathematics and Statistics (R0)