A note on stronger forms of sensitivity for inverse limit dynamical systems
- Hai Zhu^{1},
- Lei Liu^{2}Email author and
- Jian Wang^{1}
https://doi.org/10.1186/s13662-015-0425-7
© Zhu et al.; licensee Springer. 2015
Received: 20 October 2014
Accepted: 25 February 2015
Published: 28 March 2015
Abstract
In this paper we study stronger forms of sensitivity for inverse limit dynamical system which is induced from dynamical system on a compact metric space. We give the implication of stronger forms of sensitivity between inverse limit dynamical systems and original systems. More precisely, the inverse limit system is syndetically sensitive (resp. cofinitely sensitive, ergodically sensitive, multi-sensitive) if and only if original system is syndetically sensitive (resp. cofinitely sensitive, ergodically sensitive, multi-sensitive). Also, we prove that the inverse limit system is syndetically transitive if and only if original system is syndetically transitive.
Keywords
MSC
1 Introduction
Throughout this paper a topological dynamical system we mean a pair \((X,f)\), where X is a compact space and \(f:X\to X\) is a surjective continuous map. Let \(N^{+}\) denotes the set of all positive integers and let \(N=N^{+}\cup\{0\}\). When X is finite, it is a discrete space and there is no non-trivial convergence. Hence, we assume that X contains infinitely many points.
It is well known that sensitive dependence on initial conditions characterizes the unpredictability of chaotic phenomenon (see [1–12]). Sensitive dependence on initial conditions, or sensitivity for short, is the essential component of various definitions of chaos. Roughly speaking, a dynamical system \((X,f)\) is sensitive if for any open region U of the phase space, there exist two points in U and an integer \(n\in N\) such that the nth iterates of the two points under the map f are significantly separated. The largeness of the set of all \(n\in N\) where this significant separation or sensitivity happens can be thought of as a measure of how sensitive the dynamical system is. In particular, if this set is quite thin with arbitrarily large gaps between consecutive entries, then one has some excuse for treating the dynamical system as practically non-sensitive!
For continuous self-maps of compact metric spaces, Moothathu [8] initiated a preliminary study of stronger forms of sensitivity formulated in terms of large subsets of N. He considered syndetic sensitivity and cofinite sensitivity. Moreover, he constructed a transitive, sensitive map which is not syndetically sensitive and established the following. (1) Any syndetically transitive, non-minimal map is syndetically sensitive (this improves the result that sensitivity is redundant in Devaney’s definition of chaos). (2) Any sensitive map of \([0,1]\) is cofinitely sensitive. (3) Any sensitive subshift of finite type is cofinitely sensitive. (4) Any syndetically transitive, infinite subshift is syndetically sensitive. (5) No Sturmian subshift is cofinitely sensitive.
More recently, Sharma and Nagar [13] studied the relations between the various forms of sensitivity of the systems \((X,f)\) and it induced hyperspace dynamical systems \((\kappa(X),\bar{f})\). They proved that all forms of sensitivity of \((\kappa(X),\bar{f})\) partly imply the same for \((X,f)\), and the converse holds in some cases. Li et al. [14–18] introduced the notion of ergodic sensitivity which is a stronger form of sensitivity, and presented some sufficient conditions for a dynamical system \((X,f)\) to be ergodically sensitive. Also, it is shown that \((\kappa(X),\bar{f})\) is syndetically sensitive (resp. multi-sensitive) if and only if \((X,f)\) is syndetically sensitive (resp. multi-sensitive).
Along with the deep research on the properties of topological dynamical systems, many people also considered dynamical properties in some induced dynamical systems such as inverse limit dynamical systems. Li [19] studied Devaney chaos of inverse limit dynamical systems and proved that an inverse limit dynamical system is Devaney chaos if and only if its original system is Devaney chaos. Chen and Li [20] discussed shadowing property for inverse limit spaces, Ye [21] studied topological entropy of inverse limit dynamical system, Block et al. [22], Bruin [23] and Raines and Stimac [24] discussed the properties of inverse limit spaces of tent maps. Liu and Zhao [25] investigated Martelli chaos of inverse limit dynamical systems and proved that inverse limit dynamical systems were Martelli chaos implied that original systems was Martelli chaos.
In this paper we discuss stronger forms of sensitivity for inverse limit dynamical systems on the basis of [8]. Our purpose is to discuss implication of stronger forms of sensitivity between inverse limit systems and original systems. It is shown that the inverse limit system is syndetically sensitive (resp. cofinitely sensitive, ergodically sensitive, multi-sensitive) if and only if original system is syndetically sensitive (resp. cofinitely sensitive, ergodically sensitive, multi-sensitive). Also, we prove that the inverse limit system is syndetically transitive if and only if original system is syndetically transitive.
2 Preliminaries
The inverse limit space \(\lim_{\leftarrow}(X,f)\) is a compact subspace of product space \(\prod_{i=1}^{\infty}X_{i} \) (\(X_{i}=X\), \(i=1,2,\ldots\)), the shift map \(\sigma_{f}: \lim_{\leftarrow}(X,f) \to\lim_{\leftarrow}(X,f)\) is defined by \(\sigma_{f}(x_{0},x_{1},\ldots)=(f(x_{0}),x_{0},x_{1},\ldots)\). Furthermore, \(\sigma_{f}^{k}(x_{0},x_{1},\ldots)= (f^{k}(x_{0}), f^{k}(x_{1}),\ldots)\), where \(k\in N\). \(\sigma_{f}\) is a homeomorphism and \(\sigma_{f}^{-1}(x_{0},x_{1},x_{2},\ldots)=(x_{1},x_{2},\ldots)\). The inverse limit dynamical system is denoted by \((\lim_{\leftarrow}(X,f),\sigma_{f})\).
Let \((X,f)\) be a dynamical system, \(\operatorname{orb}(x,f)\) be the orbit of x under f for some \(x\in X\), i.e., \(\operatorname{orb}(x,f)=\{x, f(x), f^{2}(x),\ldots, f^{n}(x),\ldots\}\) where \(f^{n}=f\circ f^{n-1}\) and \(f^{0}\) be the identity map on X. For any two nonempty sets \(U,V\subset X\), we write \(N_{f}(U,V)=\{n\in N^{+}:U\cap f^{-n}(V)\neq \emptyset\}\).
A map \(f:X\to X\) is topologically transitive if \(N_{f}(U,V)\) is nonempty, for any nonempty open sets \(U,V\subset X\).
A subset \(S\subset N^{+}\) is thick if S contains arbitrarily large blocks of consecutive numbers. A subset \(S\subset N^{+}\) is syndetic if \(N^{+}\setminus S\) is not thick.
A map \(f:X\to X\) is syndetically transitive if \(N_{f}(U,V)\) is syndetic, for any nonempty open sets \(U,V\subset X\).
We shall use cardA to denote the cardinality of A.
f is topologically ergodic if for every pair of nonempty open sets \(U,V\subset X\), the set \(N_{f}(U,V)\) has positive upper density.
- (1)
f is sensitive if there exists a \(\delta>0\) such that for any nonempty open set \(U\subset X\), \(N_{f}(U,\delta)\) is nonempty.
- (2)
f is syndetically sensitive if there exists a \(\delta>0\) such that for every nonempty open subset \(U\subset X\), \(N_{f}(U,\delta)\) is syndetic.
- (3)
f is cofinitely sensitive if there exists a \(\delta>0\) such that for every nonempty open subset \(U\subset X\), \(N_{f}(U,\delta)\) is cofinite, that is, \(N\setminus N_{f}(U,\delta)\) is finite.
- (4)
f is ergodically sensitive if there exists a \(\delta>0\) such that for every nonempty open subset \(U\subset X\), \(N_{f}(U,\delta)\) has positive upper density.
- (5)
f is multi-sensitive if there exists \(\delta>0\) such that for every integer \(k>0\) and for any nonempty open subsets \(U_{1},U_{2},\ldots,U_{k}\subset X\), \(\bigcap_{i=1}^{k}N_{f}(U_{i},\delta)\neq\emptyset\).
- (1)
Cofinite sensitivity ⇒ multi-sensitivity.
- (2)
If \(f\times f\) is topologically transitive (this is known as topologically weak mixing), then f is multi-sensitivity.
Corollary 3 and Theorem 5 from [8] show that every Sturmian subshift is syndetically sensitive, and that no Sturmian subshift is cofinitely sensitive. In addition, Theorem 7 in [8] shows that there exists a transitive, sensitive subshift which is not syndetically sensitive. Consequently, there are sensitive transformations that are not syndetically sensitive, and syndetically sensitive maps that are not cofinitely sensitive.
Definition 2.1
Let \((X,f)\) and \((Y,g)\) be two dynamical systems. Then f and g are said to be topologically conjugate if there exists a homeomorphism \(h: X\to Y\) such that \(h\circ f=g\circ h\). The homeomorphism h is called a conjugate map.
Also, f and g are said to be topologically semiconjugate (or g is a factor of f) if \(h: X\to Y\) is a continuous surjection such that \(h\circ f=g\circ h\).
3 Main results
In this section, we shall discuss in the inverse limit spaces and find that the inverse limit dynamical system \((\lim_{\leftarrow}(X,f),\sigma_{f})\) has stronger forms of sensitivity if and only if \((X,f)\) has stronger forms of sensitivity, i.e., the inverse limit system is syndetically sensitive (resp. cofinitely sensitive, ergodically sensitive, multi-sensitive) if and only if original system is syndetically sensitive (resp. cofinitely sensitive, ergodically sensitive, multi-sensitive).
Theorem 3.1
Let \((\lim_{\leftarrow}(X,f),\sigma_{f})\) be an inverse limit dynamical system. Then f is syndetically transitive if and only if so is \(\sigma_{f}\).
Proof
Necessity. Suppose that f is syndetically transitive. We shall prove that \(N_{\sigma_{f}}(\widetilde{U},\widetilde{V})\) is a syndetic set for any nonempty open subsets \(\widetilde{U}\) and \(\widetilde{V}\) in \(\lim_{\leftarrow}(X,f)\).
Sufficiency. Suppose that \(\sigma_{f}\) is syndetically transitive. We shall prove that \(N_{f}(U,V)\) is a syndetic set for any nonempty open subsets U and V in \((X,f)\).
Let U and V be any nonempty subsets in X. Then \(\pi_{0}^{-1}(U)\) and \(\pi_{0}^{-1}(V)\) are two nonempty subsets in \(\lim_{\leftarrow}(X,f)\) because \(\pi_{0}:\lim_{\leftarrow}(X,f)\to X\) is a continuous map. Since \(\sigma_{f}\) is syndetically transitive, we have \(N_{\sigma_{f}}(\pi_{0}^{-1}(U),\pi_{0}^{-1}(V))\) is syndetic. For every \(k\in N_{\sigma_{f}}(\pi_{0}^{-1}(U),\pi_{0}^{-1}(V))\), we have \(\pi_{0}^{-1}(U)\cap\sigma_{f}^{-k}(\pi_{0}^{-1}(V))\neq\emptyset\). Since \(f^{k}\circ\pi_{0}=\pi_{0}\circ\sigma_{f}^{k}\), we have \(\pi_{0}^{-1}(U)\cap\pi_{0}^{-1}(f^{-k}(V))\neq\emptyset\), furthermore, \(\pi_{0}^{-1}(U\cap f^{-k}(V))\neq\emptyset\), which implies \(U\cap f^{-k}(V)\neq\emptyset\). Therefore, we have \(k\in N_{f}(U,V)\) and \(N_{\sigma_{f}}(\pi_{0}^{-1}(U),\pi_{0}^{-1}(V))\subset N_{f}(U,V)\). This shows that \(N_{f}(U,V)\) is syndetic, i.e., f is syndetically transitive. □
Theorem 3.2
Let \((X,f)\) be a dynamical system and \(f:X\to X\) be a surjective map. Then f is syndetically sensitive if and only if so is \(\sigma_{f}\).
Proof
Necessity. Suppose that f is syndetically sensitive with sensitive constant \(\delta>0\). We shall prove that \(N_{\sigma_{f}}(\widetilde{U},\delta)\) is syndetic for any nonempty open subset \(\widetilde{U}\) in \(\lim_{\leftarrow}(X,f)\).
Sufficiency. Suppose that \(\sigma_{f}\) is syndetically sensitive with sensitive constant \(\delta>0\). We shall prove that \(N_{f}(U,\frac{\delta}{2})\) is syndetic for any nonempty subset U in X.
Let U be a nonempty subset in X. Then \(\pi_{0}^{-1}(U)\) is a nonempty subset in \(\lim_{\leftarrow}(X,f)\) because \(\pi_{0}\) is a continuous map. Take \(\underline{x}\in\pi_{0}^{-1}(U)\), then there exists \(m>8\) such that \(B(\underline{x},\frac{\delta}{m})\subset\pi_{0}^{-1}(U)\). Since \(\sigma_{f}\) is syndetically sensitive with sensitive constant \(\delta>0\), \(N_{\sigma_{f}}(B(\underline{x},\frac{\delta }{m}),\delta)\) is syndetic. For any \(k\in N_{\sigma_{f}}(B(\underline{x},\frac{\delta }{m}),\delta)\), there exist \(\underline{x}^{*},\underline{y}^{*}\in B(\underline{x},\frac {\delta}{m})\) such that \(\underline{d}(\sigma_{f}^{k}(\underline{x}^{*}), \sigma_{f}^{k}(\underline {y}^{*}))>\delta\). Since \(\sigma_{f}^{k-1}\) is continuous for \(\underline{x}\), there exists \(\frac{\delta}{m}<\delta'<\frac{\delta}{8}\), when \(\underline{x}'\in B(\underline{x},\delta')\), we have \(\underline{d}(\sigma_{f}^{k-1}(\underline{x}'),\sigma _{f}^{k-1}(\underline{x}))<\frac{\delta}{8}\). By the triangular inequality, \(\underline{d}(\sigma_{f}^{k-1}(\underline{x}^{*}),\sigma_{f}^{k-1}(\underline {y}^{*}))<\frac{\delta}{4}\).
Theorem 3.3
Let \((X,f)\) be a dynamical system and \(f:X\to X\) be a surjective map. Then f is cofinitely sensitive if and only if so is \(\sigma_{f}\).
Proof
Necessity. Suppose that f is cofinitely sensitive with sensitive constant \(\delta>0\). We shall prove that \(N_{\sigma_{f}}(\widetilde{U},\delta)\) is cofinite for any nonempty open subset \(\widetilde{U}\) in \(\lim_{\leftarrow}(X,f)\).
Sufficiency. Suppose that \(\sigma_{f}\) is cofinitely sensitive with sensitive constant \(\delta>0\). We shall prove that \(N_{f}(U,\frac{\delta}{2})\) is cofinite for any nonempty subset U in X.
Let U be a nonempty subset in X. Then \(\pi_{0}^{-1}(U)\) is a nonempty subset in \(\lim_{\leftarrow}(X,f)\) because \(\pi_{0}\) is a continuous map. Take \(\underline{x}\in\pi_{0}^{-1}(U)\), then there exists \(m>8\) such that \(B(\underline{x},\frac{\delta}{m})\subset\pi_{0}^{-1}(U)\). Since \(\sigma_{f}\) is cofinitely sensitive with sensitive constant \(\delta>0\), then \(N_{\sigma_{f}}(B(\underline{x},\frac{\delta }{m}),\delta)\) is cofinite. For any \(k\in N_{\sigma_{f}}(B(\underline{x},\frac{\delta }{m}),\delta)\), there exist \(\underline{x}^{*},\underline{y}^{*}\in B(\underline{x},\frac {\delta}{m})\) such that \(\underline{d}(\sigma_{f}^{k}(\underline{x}^{*}), \sigma_{f}^{k}(\underline {y}^{*}))>\delta\). Since \(\sigma_{f}^{k-1}\) is continuous for \(\underline{x}\), then there exists \(\frac{\delta}{m}<\delta'<\frac{\delta}{8}\), when \(\underline{x}'\in B(\underline{x},\delta')\), we have \(\underline{d}(\sigma_{f}^{k-1}(\underline{x}'),\sigma _{f}^{k-1}(\underline{x}))<\frac{\delta}{8}\). By the triangular inequality, \(\underline{d}(\sigma_{f}^{k-1}(\underline{x}^{*}),\sigma_{f}^{k-1}(\underline {y}^{*}))<\frac{\delta}{4}\).
Theorem 3.4
Let \((X,f)\) be a dynamical system and \(f:X\to X\) be a surjective map. Then f is ergodically sensitive if and only if so is \(\sigma_{f}\).
Proof
Necessity. Suppose that f is ergodically sensitive with sensitive constant \(\delta>0\). We shall prove that \(N_{\sigma_{f}}(\widetilde{U},\delta)\) has positive upper density for any nonempty open subset \(\widetilde{U}\) in \(\lim_{\leftarrow}(X,f)\).
Sufficiency. Suppose that \(\sigma_{f}\) is ergodically sensitive with sensitive constant \(\delta>0\). We shall prove that \(N_{f}(U,\frac{\delta}{2})\) has positive upper density for any nonempty subset U in X.
Theorem 3.5
Let \((X,f)\) be a dynamical system and \(f:X\to X\) be a surjective map. Then f is multi-sensitive if and only if so is \(\sigma_{f}\).
Proof
Necessity. Suppose that f is multi-sensitive with sensitive constant \(\delta>0\). We shall prove that \(\bigcap_{i=1}^{p}N_{\sigma _{f}}(\widetilde{U}_{i},\delta)\neq\emptyset\) for every \(p\in N\) and any nonempty open subset \(\widetilde{U}_{i}\) (\(i=1,2,\ldots,p\)) in \(\lim_{\leftarrow}(X,f)\).
Sufficiency. Suppose that \(\sigma_{f}\) is multi-sensitive with sensitive constant \(\delta>0\). We shall prove that \(\bigcap_{i=1}^{p}N_{f}(U_{i},\frac{\delta}{2})\neq\emptyset\) for any nonempty open subset \(U_{i}\) (\(i=1,2,\ldots,p\)) in X.
Let \(U_{i}\) (\(i=1,2,\ldots,p\)) be a nonempty open subset in X. Then \(\pi _{0}^{-1}(U_{i})\) is a nonempty open subset in \(\lim_{\leftarrow}(X,f)\) because \(\pi_{0}\) is a continuous map. Take \(\underline{x_{i}}\in\pi_{0}^{-1}(U_{i})\), then there exists \(m>8\) such that \(B(\underline{x_{i}},\frac{\delta}{m})\subset\pi_{0}^{-1}(U_{i})\) for \(i=1,2,\ldots,p\). Since \(\sigma_{f}\) is multi-sensitive with sensitive constant \(\delta>0\), we have \(\bigcap_{i=1}^{p}N_{\sigma_{f}}(B(\underline{x_{i}},\frac{\delta }{m}),\delta)\neq\emptyset\). For any \(k\in N_{\sigma_{f}}(B(\underline{x_{i}},\frac{\delta}{m}),\delta)\) (\(i=1,2,\ldots,p\)), there exist \(\underline{x^{*}_{i}},\underline{y^{*}_{i}}\in B(\underline {x},\frac{\delta}{m})\) such that \(\underline{d}(\sigma_{f}^{k}(\underline{x^{*}_{i}}),\sigma_{f}^{k}(\underline {y^{*}_{i}}))>\delta\). Since \(\sigma_{f}^{k-1}\) is continuous for \(\underline{x_{i}}\), there exists \(\frac{\delta}{m}<\delta'<\frac{\delta}{8}\), when \(\underline{x'_{i}}\in B(\underline{x_{i}},\delta')\), we have \(\underline{d}(\sigma_{f}^{k-1}(\underline{x'_{i}}),\sigma _{f}^{k-1}(\underline{x_{i}}))<\frac{\delta}{8}\) for \(i=1,2,\ldots,p\). By the triangular inequality, \(\underline{d}(\sigma_{f}^{k-1}(\underline{x^{*}_{i}}),\sigma _{f}^{k-1}(\underline{y^{*}_{i}}))<\frac{\delta}{4}\) for \(i=1,2,\ldots,p\).
Declarations
Acknowledgements
We would like to thank the reviewers for their constructive comments and valuable suggestions. The work was supported by the National Natural Science Foundation of China (11401363, 61103143), China Postdoctoral Science Foundation funded project (2012M512008), Program for Science & Technology Innovation Talents in Universities of Henan Province (2012HASTIT032) and the Education Foundation of Henan Province (13A110832, 14B110006), P.R. China. The authors would like to thank the referees for many valuable and constructive comments and suggestions for improving this paper.
Open Access This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.
Authors’ Affiliations
References
- Abraham, C, Biau, G, Cadre, B: Chaotic properties of mapping on a probability space. J. Math. Anal. Appl. 266, 420-431 (2002) View ArticleMATHMathSciNetGoogle Scholar
- Banks, J, Brooks, J, Cairns, G, Davis, G, Stacey, P: On Devaney’s definition of chaos. Am. Math. Mon. 99, 332-334 (1992) View ArticleMATHMathSciNetGoogle Scholar
- Glasner, E, Weiss, B: Sensitive dependence on initial conditions. Nonlinearity 6, 1067-1075 (1993) View ArticleMATHMathSciNetGoogle Scholar
- Gu, RB: The large deviations theorem and ergodicity. Chaos Solitons Fractals 34, 1387-1392 (2007) View ArticleMATHMathSciNetGoogle Scholar
- He, LF, Yan, XH, Wang, LS: Weak-mixing implies sensitive dependence. J. Math. Anal. Appl. 299, 300-304 (2004) View ArticleMATHMathSciNetGoogle Scholar
- Kato, H: Everywhere chaotic homeomorphisms on manifolds and k-dimensional Merger manifolds. Topol. Appl. 72, 1-17 (1996) View ArticleMATHGoogle Scholar
- Lardjane, S: On some stochastic properties in Devaney’s chaos. Chaos Solitons Fractals 28, 668-672 (2006) View ArticleMATHMathSciNetGoogle Scholar
- Moothathu, TKS: Stronger forms of sensitivity for dynamical systems. Nonlinearity 20, 2115-2126 (2007) View ArticleMATHMathSciNetGoogle Scholar
- Shao, S, Ye, XD, Zhang, RF: Sensitivity and regionally proximal relation in minimal systems. Sci. China Ser. A 51, 987-994 (2008) (in Chinese) View ArticleMATHMathSciNetGoogle Scholar
- Wu, C, Xu, ZJ, Lin, W, Ruan, J: Stochastic properties in Devaney’s chaos. Chaos Solitons Fractals 23, 1195-1199 (2005) View ArticleMATHMathSciNetGoogle Scholar
- Xu, ZJ, Lin, W, Ruan, J: Decay of correlations implies chaos in the sense of Devaney. Chaos Solitons Fractals 22, 305-310 (2004) View ArticleMATHMathSciNetGoogle Scholar
- Ye, XD, Zhang, RF: On sensitive sets in topological dynamics. Nonlinearity 21, 1601-1620 (2008) View ArticleMATHMathSciNetGoogle Scholar
- Sharma, P, Nagar, A: Inducing sensitivity on hyperspaces. Topol. Appl. 157, 2052-2058 (2010) View ArticleMATHMathSciNetGoogle Scholar
- Li, RS: A note on stronger forms of sensitivity for dynamical systems. Chaos Solitons Fractals 45, 753-758 (2012) View ArticleMATHMathSciNetGoogle Scholar
- Li, RS: A note on shadowing with chain transitivity. Commun. Nonlinear Sci. Numer. Simul. 17, 2815-2823 (2012) View ArticleMATHMathSciNetGoogle Scholar
- Li, RS: The large deviations theorem and ergodic sensitivity. Commun. Nonlinear Sci. Numer. Simul. 18, 819-825 (2013) View ArticleMATHMathSciNetGoogle Scholar
- Li, RS, Shi, YM: Stronger forms of sensitivity for measure-preserving maps and semiflows on probability spaces. Abstr. Appl. Anal. 2014, Article ID 769523 (2014) Google Scholar
- Li, RS, Zhou, XL: A note on chaos in product maps. Turk. J. Math. 37, 665-675 (2013) View ArticleMATHGoogle Scholar
- Li, S: Dynamical properties of the shift maps on the inverse limit spaces. Ergod. Theory Dyn. Syst. 12, 95-108 (1992) View ArticleMATHGoogle Scholar
- Chen, L, Li, SH: Shadowing property for inverse limit space. Proc. Am. Math. Soc. 115, 573-580 (1992) View ArticleMATHGoogle Scholar
- Ye, XD: Topological entropy of the induced maps of the inverse limits with bonding maps. Topol. Appl. 67, 113-118 (1995) View ArticleMATHGoogle Scholar
- Block, L, Jakimovik, S, Keesling, J, Kailhofer, L: On the classification of inverse limits of tent maps. Fundam. Math. 187, 171-192 (2005) View ArticleMATHMathSciNetGoogle Scholar
- Bruin, H: Inverse limit spaces of post-critically finite tent maps. Fundam. Math. 165, 125-138 (2000) MATHMathSciNetGoogle Scholar
- Raines, B, Stimac, S: A classification of inverse limit spacers of tent maps with non-recurrent critical point. Algebr. Geom. Topol. 9, 1049-1088 (2009) View ArticleMATHMathSciNetGoogle Scholar
- Liu, L, Zhao, SL: Martelli’s chaos in inverse limit dynamical systems and hyperspace dynamical systems. Results Math. 63, 195-207 (2013) View ArticleMATHMathSciNetGoogle Scholar