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Limit dynamics of elementary cellular automaton 18

Published online by Cambridge University Press:  20 April 2026

EMILIE SABRIÉ
Affiliation:
Computer Science Department, ENS-Paris Saclay , France (e-mail: herve.sabrie@ens-paris-saclay.fr)
ILKKA ALEKSI TÖRMÄ*
Affiliation:
Department of Mathematics and Statistics, University of Turku , Finland
*
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Abstract

We study the the asymptotic dynamics of elementary cellular automaton 18 through its limit set, generic limit set and $\mu $-limit set. The dynamics of rule 18 are characterized by persistent local patterns known as kinks. We characterize the configurations of the generic limit set containing at most two kinks. As a corollary, we show that the three limit sets of rule 18 are distinct.

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Type
Original Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited.
Copyright
© The Author(s), 2026. Published by Cambridge University Press
Figure 0

Table 1 The local rule of ECA 18.Table 1 long description.

Figure 1

Figure 1 An example run of rule 18. The centre of each kink is marked with a circle.Figure 1 long description.

Figure 2

Figure 2 The word u1$u_1$ above contains an even number of kinks; hence, f(u1)$f(u_1)$ is not a kink. The word u2$u_2$ below contains an odd number of kinks; hence, f(u2)$f(u_2)$ is a kink.Figure 2 long description.

Figure 3

Figure 3 Two kinks collide and annihilate each other, but it is possible to avoid collision by making the leftmost kink longer.Figure 3 long description.

Figure 4

Figure 4 We can see here that w=0010101100101$w = 0010101100101$ is stable, f(w)$f(w)$ and f2(w)$f^2(w)$ are stable, and f3(w)=1001011$f^3(w) = 1001011$. We can deduce that Σ(1001011)=f3(Σ(w))⊆f3(Σ(1001011))$\Sigma (1001011) = f^3(\Sigma (w)) \subseteq f^3(\Sigma (1001011))$.

Figure 5

Figure 5 We can see here that w=1010010110100$w = 1010010110100$ is stable, f(w)$f(w)$ and f2(w)$f^2(w)$ are stable, and f3(w)=1101001$f^3(w) = 1101001$. We can deduce that Σ(1101001)=f3(Σ(w))⊆f3(Σ(1001011))$\Sigma (1101001) = f^3(\Sigma (w)) \subseteq f^3(\Sigma (1001011))$.

Figure 6

Figure 6 We can see here that w=00101100001$w = 00101100001$ is stable, f(w)$f(w)$ is stable and f2(w)=1001011$f^2(w) = 1001011$. We can deduce that Σ(1101001)⊆f2(Σ(1001011))=f5(Σ(w))⊆f5(Σ(1100001))$\Sigma (1101001) \subseteq f^2(\Sigma (1001011)) = f^5(\Sigma (w)) \subseteq f^5(\Sigma (1100001))$.

Figure 7

Figure 7 We can see here that w=00001011000110101000100$w = 00001011000110101000100$ is stable, f(w),f2(w),…,f7(w)$f(w), f^2(w), \ldots , f^7(w)$ are stable and f8(w)=1101001$f^8(w) = 1101001$. We can deduce that Σ(1101001)=f8(Σ(w))⊆f8(Σ(1100011))$\Sigma (1101001) = f^8(\Sigma (w)) \subseteq f^8(\Sigma (1100011))$.Figure 7 long description.

Figure 8

Figure 8 At each step of the backward computation, we force the four left and four right symbols to be either 0110$0110$ or 1001$1001$, this in turn fixes the neighbours symbols to some value. After enough steps, the whole word is forced.Figure 8 long description.

Figure 9

Figure 9 In the same way as in Figure 8, after enough steps of backward computation, the whole word is forced.Figure 9 long description.

Figure 10

Figure 10 Moving a 1101001$1101001$ one step to the left.

Figure 11

Figure 11 Moving a 1101001$1101001$ one step to the right.