11 research outputs found

    Dynamics and Topology of S-gap Shifts

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    Let S={si∈N∪{0}:0≤si<si+1}S=\{s_i\in\mathbb N\cup\{0\}:0\leq s_i<s_{i+1}\} and let d0=s0d_{0}=s_{0} and Δ(S)={dn}n\Delta(S)=\{d_{n}\}_{n} where dn=sn−sn−1d_{n}=s_{n}-s_{n-1}. In this note, we show that an SS-gap shift is subshift of finite type (SFT) if and only if SS is finite or cofinite, is almost-finite-type (AFT) if and only if Δ(S)\Delta(S) is eventually constant and is sofic if and only if Δ(S)\Delta(S) is eventually periodic. We also show that there is a one-to-one correspondence between the set of all SS-gap shifts and {r∈R:r≥0}\{1n:n∈N}\{r \in \mathbb R: r \geq 0\}\backslash \{\frac{1}{n}: n \in {\mathbb N}\} up to conjugacy. This enables us to induce a topology and measure structure on the set of all SS-gaps. By using this, we give the frequency of certain SS-gap shifts with respect to their dynamical properties.Comment: This paper has been withdrawn due to a flaw in Theorem 3.2. The correct version with some minor results will be replace

    Computations on Sofic S-gap Shifts

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    Let S={sn}S=\{s_{n}\} be an increasing finite or infinite subset of N⋃{0}\mathbb N \bigcup \{0\} and X(S)X(S) the SS-gap shift associated to SS. Let fS(x)=1−∑1xsn+1f_{S}(x)=1-\sum\frac{1}{x^{s_{n}+1}} be the entropy function which will be vanished at 2h(X(S))2^{h(X(S))} where h(X(S))h(X(S)) is the entropy of the system. Suppose X(S)X(S) is sofic with adjacency matrix AA and the characteristic polynomial χA\chi_{A}. Then for some rational function QS Q_{S} , χA(x)=QS(x)fS(x)\chi_{A}(x)=Q_{S}(x)f_{S}(x). This QS Q_{S} will be explicitly determined. We will show that ζ(t)=1fS(t−1)\zeta(t)=\frac{1}{f_{S}(t^{-1})} or ζ(t)=1(1−t)fS(t−1)\zeta(t)=\frac{1}{(1-t)f_{S}(t^{-1})} when ∣S∣<∞|S|<\infty or ∣S∣=∞|S|=\infty respectively. Here ζ\zeta is the zeta function of X(S)X(S). We will also compute the Bowen-Franks groups of a sofic SS-gap shift.Comment: This paper has been withdrawn due to extending results about SFT shifts to sofic shifts (Theorem 2.3). This forces to apply some minor changes in the organization of the paper. This paper has been withdrawn due to a flaw in the description of the adjacency matrix (2.3
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