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ENTROPY, MIXING PROPERTIES, AND LI–YORKE CHAOS OF MONOID ACTIONS

Published online by Cambridge University Press:  20 April 2026

JUNG-CHAO BAN
Affiliation:
Department of Mathematical Sciences, National Chengchi University , Taipei 11605, Taiwan, ROC and Math. Division, National Center for Theoretical Science, National Taiwan University, Taipei 10617, Taiwan, ROC e-mail: jcban@nccu.edu.tw
GUAN-YU LAI
Affiliation:
Department of Natural Science in the Center for General Education, Chang Gung University , Taoyuan 333323, Taiwan, ROC e-mail: gylai@cgu.edu.tw
CHENG-YU TSAI*
Affiliation:
Department of Mathematical Sciences, National Chengchi University , Taipei 11605, Taiwan, ROC
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Abstract

In this paper, we investigate dynamical properties of monoid actions on symbolic systems. First, we establish mixing properties and an entropy formula for such actions. To describe chaotic behavior, we introduce and distinguish several types of Li–Yorke chaos. Our main result shows that positive entropy is equivalent to locally Li–Yorke chaos, a notion that strengthens the classical definition of Li–Yorke chaos.

MSC classification

Information

Type
Research Article
Copyright
© The Author(s), 2026. Published by Cambridge University Press on behalf of Australian Mathematical Publishing Association Inc.
Figure 0

Figure 1 The graph of ΣM∗$\Sigma _M^*$ with M$ M $ is defined in (4-1).Figure 1 long description.

Figure 1

Figure 2 The graph of the Markov tree-shift T=TΣM∗$T=T_{\Sigma _M^*}$ associated with a family R$\mathcal {R}$ of relations, determined by (A1,A2,A3)$(A_1,A_2,A_3)$ and the matrix M$ M $ is defined in (4-1).

Figure 2

Figure 3 The graph shows the values of |ΣM≤n|−1log⁡|TΣM≤n|$|\Sigma _M^{\leq n}|^{-1}\log | T_{\Sigma _M^{\leq n}}|$ for 1≤n≤100$1\leq n\leq 100$. The quantity |TΣM≤n|$|T_{\Sigma _M^{\leq n}}|$ is a function of a family R$\mathcal {R}$ of relations (that is |TΣM≤n|=|TΣM≤n(R)|)$(\text {that is }|T_{\Sigma _M^{\leq n}}|=|T_{\Sigma _M^{\leq n}}(\mathcal {R})|)$, where the family R1$\mathcal {R}_1$ (respectively R2$\mathcal {R}_2$, R3$\mathcal {R}_3$, R4$\mathcal {R}_4$) is determined by (E,[1 0;0 1],E)(respectively (E,[1 0;1 1],E),(E,E,E),(E,[1 1;1 0],[1 1;1 0]))$(E,[1~0;0~1],E)\, (\text {respectively } (E,[1~0;1~1],E),(E,E,E),(E,[1~1;1~0],[1~1;1~0]) )$.Figure 3 long description.

Figure 3

Table 1 Entropy of TΣM∗$T_{\Sigma_M^*}$: numerical approximations and exact values.Table 1 long description.

Figure 4

Figure 4 The graph of a Markov tree-shift T=TΣM∗$T=T_{\Sigma _M^*}$ associated with a family R$\mathcal {R}$ of relations, determined by (A1,A2)$(A_1,A_2)$, and the matrix M is defined in (4-11).

Figure 5

Figure 5 The graph of a Markov tree-shift T has its root labeled a.