Modelled as finite homogeneous Markov chains, probabilistic cellular automata with local transition probabilities in (0, 1) always posses a stationary distribution. This result alone is not very helpful when it comes to predicting the final configuration; one needs also a formula connecting the probabilities in the stationary distribution to some intrinsic feature of the lattice configuration. Previous results on the asynchronous cellular automata have showed that such feature really exists. It is the number of zero-one borders within the automaton's binary configuration. An exponential formula in the number of zero-one borders has been proved for the 1-D, 2-D and 3-D asynchronous automata with neighborhood three, five and seven, respectively. We perform computer experiments on a synchronous cellular automaton to check whether the empirical distribution obeys also that theoretical formula. The numerical results indicate a perfect fit for neighbourhood three and five, which opens the way for a rigorous proof of the formula in this new, synchronous case.
Citation: Agapie A, Andreica A, Chira C, Giuclea M (2014) Predictability in Cellular Automata. PLoS ONE 9(10): e108177. https://doi.org/10.1371/journal.pone.0108177
Editor: Jesus Gomez-Gardenes, Universidad de Zarazoga, Spain
Received: April 6, 2014; Accepted: July 28, 2014; Published: October 1, 2014
Copyright: © 2014 Agapie et al. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
Data Availability: The authors confirm that all data underlying the findings are fully available without restriction. All relevant data are within the paper and its Supporting Information files.
Funding: Funding provided by AA PNII-ID-PCCE-2011-0015, Romanian National Authority for Scientific Research, http://uefiscdi.gov.ro/, AA Grant PNII-TE-320, Romanian National Authority for Scientific Research, http://uefiscdi.gov.ro/ and CC Grant PNII-TE-320, Romanian National Authority for Scientific Research, http://uefiscdi.gov.ro/. The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.
Competing interests: The authors have declared that no competing interests exist.
From a mathematical point of view, cellular automata (CA) are binary lattices that are updated iteratively. In the automata discussed in this paper, the value of a cell is flipped based only on the number of ones in the neighborhood of the cell to be updated. We call an automaton synchronous if all cells are updated simultaneously, respectively asynchronous if the updating affects only one cell at a time.
• the updated cell is picked at random
• the local transition rule is probabilistic - e.g., a cell may flip from zero to one with some probability , and the same cell may stay in zero with probability .
Probabilistic automata are suitable for Markov chain modelling, since the future configuration of the automaton depends only on its present state.
A finite homogeneous Markov chain is a stochastic process that moves according to some probabilities within a finite set of states, say , with transition probability from state to state (denoted ) depending only on states and . The square, non-negative transition matrix gathers all the above transition probabilities. Transition matrix of a Markov chain is always stochastic - that is, the sum of probabilities in each row is one, and since in our case the matrix does not change from an iteration to another, it is called homogeneous.
Definition 0.1. • A state is absorbing if . An absorbing state is never left, once it is entered.
• A stochastic matrix is primitive if there is a positive integer such that is (strictly) positive.
• A stochastic matrix is called stable if all its rows are identical.
• Let be a probability vector. If is the initial distribution of the Markov chain with transition matrix , then the distribution after steps is , with , for all . If , then is a stationary distribution.
Theorem 0.2. Let be a primitive transition matrix. Then converges as to a positive stable stochastic matrix , and the rate of approach to the limit is geometric. Moreover, the limit distribution has the following properties:
• is unique regardless of the initial distribution ;
• has positive entries on all components;
• is also the unique stationary distribution of the associated Markov chain.
There are many problems of interest in Markov chain theory . The short-term behavior implies the correct definition of the transition matrix to be associated to some process. The long term-behavior is even more important, opening the way for prediction; that is strictly connected to the stationary distribution, and to finding necessary and sufficient conditions that guarantee its existence. Providing the stationary distribution in elegant, analytical form would be a bonus - fortunately, this is the case in our study. Finally, estimating the time the chain takes until convergence is also of interest - this topic is usually referred to in literature as absorption time.
When it comes to CA, literature has focused so far only on the first two topics. The computation of absorption time is also of certain interest, at least for the class of deterministic automata with two attractors, all zeros and all ones.
Deterministic Cellular Automata
The monograph of Wolfram  and the papers of Chua and co-workers ,  are referential works in deterministic CA literature. While Wolfram's pursuit of explaining complexity uses the empirical analysis of automata as a vehicle, Chua and co-workers put on mathematically sound clothes to Wolfram's original approach, in form of nonlinear differential equations , . To make things clear, let us see first a particular CA at work.
Consider a two-state CA (the values of the states are set to 0 and 1 within this paper) with cells and circular connection - the left-hand neighbor of cell is cell . Cell is influenced only by itself and its nearest neighbors and . The values of cells , and are the input of the process that is going to change cell . Such system is called 1-D three-neighborhood CA.
In the deterministic case, each of the eight possible input configurations yields a certain output for the central cell . There are different functions and each of these functions will be assimilated to a local rule. If we denote , we have a one to one mapping between the 256 functions and the set of Boolean vectors . It is thus natural to identify each of the 256 functions by its associated decimal representation (1)
For example, the famous rule 110 - proved to be a universal Touring machine  - is defined synthetically by the Boolean vector , and explicitly by table 1. Notice that input consists of the whole three-neighborhood, while output is the new value of the central cell.
It is hard to find an intuitive interpretation of rule 110. Indeed, neither majority, nor minority governs the CA in table 1: would indicate a majority rule, while points otherwise.
That is not the case with rule 232, which clearly defines a majority decision model, table 2.
While Wolfram studied the 256 rules empirically, by running extensive computer experiments , Chua and co-workers proved rigorously that more insight into CA dynamic behavior can be gained by associating local rules like the one above to the attractors of so-called cellular neural networks (CNN).
As introduced in , CNN is a finite string with circular connection, and a nonlinear dynamical system acting on each cell , defined by a state equation(2)and an output equation(3)
Equation (3) provides the steady state output Q of cell for each neighborhood input of type , yet with symbol ‘0’ replaced by ‘-1’, e.g. becomes . For each deterministic local rule, one can set the parameters in the above equations such that the trajectory converges to an attractor Q with output generating the -1/1 correspondent of the Boolean vector associated to the rule itself. For example, the state and output equations in case of rule 110 read(4)
Equations (2)-(3) define only one CA iteration. According to , one can use a CNN chip to simulate ‘physically’ a local rule on all cells simultaneously. Therefore, one can describe each local rule as a nonlinear difference equation(5)
In , Wolfram starts from a fixed initial initial configuration , runs the 61-cell deterministic CA for each of the 256 local rules, independently, stores the produced configurations in large bi-colour arrays, then looks for similar patterns among arrays corresponding to different rules. He proves that rule 110 is universal Touring machine and, based on the geometrical similarity, conjectures that three other rules, namely 124, 137 and 193 are also universal Touring machines.
Using Felix Klein's Vierergruppe V, Chua and co-workers obtain a classification of the 256 rules into 89 global equivalence classes . Rules 110, 124, 137 and 193 fall into the same class, which gives a rigorous proof to Wolfram's conjecture. From a nonlinear dynamics point of view, these four rules are identical. As for the majority rule 232, it forms a class by its own, there are no other rules equivalent to it. Another interesting application of this analysis is to the problem of density classification, see e.g. .
Probabilistic Cellular Automata
In order to describe a probabilistic CA consider the 1-D three neighborhood automaton from the previous section, but with some randomness added to the local transition rule.
Consider first the model of an asynchronous CA - only one cell is flipped (at most) per iteration. We pick the cell for the flip uniformly - each cell with equal probability . Once selected, the value of cell changes according to some local probabilities, depending on the number of ones within the significant neighborhood , see table 3, where are the two parameters of the model.
Table 3 considers all possible transitions, even the virtual ones. For instance, if value of cell is and there are two ones in the current neighborhood, cell will ‘transit’ to with probability . In other words, transition is still considered a flip. Compared to Wolfram's model of deterministic CA, the probabilistic model of table 3 allows for a unitary interpretation of local rules. Indeed, it makes no difference between local configurations and as they both have two ones, yet that does not mean that the middle cell will transit to the same value - it still depends on randomness.
The Markov model of the asynchronous three-neighborhood automaton has been introduced in . There are states in the Markov chain, consisting of all binary configurations of length . For an arbitrary state - here denotes a CA configuration, not a single cell - there are precisely positive entries in row of the global transition matrix, namely the (global) transitions to states that differ from on a single cell, plus the element on the main diagonal.
The off-diagonal probabilities take values from the set depending on the distribution of cells in the significant neighborhood of the cell in that should undergo a flip to get . The diagonal probability is equal to one minus all off-diagonal probabilities in row . Since for , transition matrix is primitive. Then theorem 0.2 guarantees the existence of the limit distribution, also the (unique) stationary distribution of the Markov chain.
We found formulas for the stationary distribution of various asynchronous cellular automata , , , and we connected our findings to existent results from Ising and exponential voter model . The most important results are presented in the following.
Definition 0.3. A border occurs in a CA configuration between two different successive cells, like in 01 or 10. The total number of borders within configuration is denoted .
Next theorem induces a class property on the set of configurations, revealing the stationary distribution as function of the number of borders.
The computation of is solved by the following.
Lemma 0.5. The number of configurations with borders is , for all .
Before moving further let us explain the practical meaning of the above results. The stationary distribution of the automaton is a probability vector with strictly positive components. That means the CA will not converge to a single state, but it will journey through all states, the sojourn time of each state being proportional to the corresponding probability in the stationary distribution. The succession of states in the journey remains unpredictable. What we can predict is that some configurations will have larger sojourn times than others, and formula (7) maps the sojourn time of a configuration to an exponential function of the number of borders within that configuration. Lemma 0.5 shows how many configurations fall in each class. Within a particular class, all configurations have exactly the same probability in the stationary distribution, thus their sojourn times will be the same.
It is also worth mentioning that the initial CA configuration does not influence the long term behavior of the probabilistic automaton, since the stationary distribution is independent of the Markov chain's starting point.
The majority model fulfils , so the basis of the exponential function (7) is sub-unitary, and the larger the number of borders within a configuration, the smaller the time spent by the automaton in that configuration. Consequently, configurations all zeros and all ones, which both belong to class , have the largest sojourn times, while configurations and (with maximal number of borders) have the smallest sojourn times. Needless to say, situation reverses completely if .
In case of the five-neighborhood CA, there is one more parameter involved, call it , table 4, and the generalization of theorem (0.4) requires a supplementary condition on , and , which ensures the so-called detailed balance equation.
A refinement of the border definition is first needed.
Definition 0.6. A k-border occurs between two different cells situated at distance from each other. E.g., in we have a 2-border between first and third cell, and a 1-border between second and third cell.
An analogous of lemma 0.5 also holds.
Using computer experiments we test the generality of the stationary distributions from previous section. Our assumption is that synchronous automata obey the same probability laws as their asynchronous counterparts. In order to build a synchronous CA, we drop the ‘only one cell per iteration undergoes a flip’ condition, and update all the cells in the same iteration, one by one from left to right.
For each numerical simulation we run CA iterations starting from an arbitrary configuration and store the next iterations in order to build an empirical stationary distribution - ranges between and .
Consider the three-neighborhood automaton. Formula (7) stands for the theoretical distribution, with constant provided by lemma 0.5. We set local probabilities to and , and the length of CA to ; that yields the following partition of the configuration space w.r.t. the number of borders: .
Figure 1 shows a perfect match between the theoretical distribution and the empirical distribution of asynchronous CA, with and , respectively. The value of has no influence on the numerical results.
We consider next the five-neighborhood CA. The following lemma explains the partition of the configuration space in this case.
Lemma 0.9. The partition induced by formula (10) on the five-neighborhood CA with length is given in table 5.
Proof. We need to consider all possible cases w.r.t. the sum of order-1 and order-2 borders, and for each case we should count the configurations with formula (10). Notice that the number of borders is always even, regardless of the order.
There are only two configurations in this class, namely all zeros and all ones.
One can easily check that this class is empty: there is no configuration with 2 order-1 and 0 order-2 borders, nor vice versa.
Summing up the number of configurations in each class completes the proof.
Basically, we performed the same tests as for the three-neighborhood automaton, with . There is a difference, though. Theorem 0.7 provides the exponential form of the stationary distribution, but only under condition (8), which ensures detailed balance equation for the associated Markov chain. So it makes sense to test numerically whether this condition is really necessary. We present below results for the five-neighborhood synchronous CA, under two different settings of local transition probabilities: one arbitrary, , not fulfilling (8), and the other, , in perfect agreement with (8) and denoted DBE in figure 2. For Theory we used the theoretical stationary distribution (9) of the asynchronous case. The fact that the empirical distribution of the automaton with arbitrary local probabilities is far from the theoretical formula proves that condition (8) can not be removed.
Classification and prediction are the key issues in cellular automata. In the deterministic case, Wolfram relied on the inspiration of a computer analyst to derive patterns from the experimental simulation of different local rules. Chua and co-workers took the analysis a step further by demonstrating rigorously that every local rule can be mapped to a nonlinear dynamical system whose attractors encode accurately that very rule.
The situation is different with Markov chains. Here, predictability takes the form of the stationary distribution, which gathers the long-term sojourn times of each and every state of the system under consideration. For large systems like cellular automata, the existence of the stationary distribution alone is not very helpful, unless we have also an analytic formula able to connect the probabilities in the stationary distribution to some intrinsic features of the automaton configurations. Such fortunate situation is demonstrated in the paper, with an exponential stationary distribution, function of the number of borders within the configuration. The formulas, rigorously proved in previous papers for the asynchronous case, have been successfully tested via computer simulation on synchronous automata.
So far, the validation is only numerical, but the very good agreement between the (theoretical) formula and the (empirical) stationary distribution of synchronous automaton is a clear indication of the generality of the formula. As usually the case in theoretical computer science, the experimental results open the way for rigorous mathematical proofs, as well as for enlarging the test-bed by considering different variants of cellular automata. Another direction for future research is the stochastic analysis of absorption time, in case of the automata converging to the extreme configurations all zeros and all ones.
Conceived and designed the experiments: A. Agapie A. Andreica. Performed the experiments: CC. Analyzed the data: MG. Contributed reagents/materials/analysis tools: A. Andreica. Wrote the paper: A. Agapie A. Andreica CC MG.
- 1. Agapie A (2010) Simple form of the stationary distribution for 3D cellular automata in a special case. Physica A 389: 2495–2499.
- 2. Agapie A, Höns R, Agapie Ad (2010) Limit behavior of the exponential voter model. Mathematical Social Sciences 59: 271–281.
- 3. Agapie A, Aus der Fuenten T (2008) Stationary distribution for a majority voter model. Stochastic Models 24: 503–512.
- 4. Agapie A, Mühlenbein H, Höns R (2004) Markov Chain Analysis for One-Dimensional Asynchronous Cellular Automata. Methodology and Computing in Applied Probability 6: 181–201.
- 5. Chua LO, Yoon S, Dogaru R (2002) A nonlinear dynamics perspective of Wolframs new kind of science. Part III: Predicting the Unpredictable. Int J Bifurcation and Chaos 14: 3689–3820.
- 6. Chua LO, Yoon S, Dogaru R (2002) A nonlinear dynamics perspective of Wolframs new kind of science. Part I: Threshold of complexity. Int J Bifurcation and Chaos 12: 26552766.
- 7. Clifford P, Sudbury A (1973) A model for spatial conflict. Biometrika 60: 581–588.
- 8. Durrett R (1988) Lecture Notes on Particle Systems and Percolation. Wadsworth
- 9. Gog A, Chira C (2009) Cellular Automata Rule Detection Using Circular Asynchronous Evolutionary Search. Lecture Notes in Computer Science 5572: 261–268.
- 10. Iosifescu M (2007) Finite Markov Processes and Applications. Dover New York.
- 11. Holley R, Liggett TM (1975) Ergodic theorems for weakly interacting systems and the voter model. Ann Probab 3: 643–663.
- 12. Liggett TM (2005) Interacting Particle Systems. Springer New York.
- 13. Parzen E (1999) Stochastic Processes. SIAM Philadelphia.
- 14. Seneta E (1981) Non-negative Matrices and Markov Chains. New York Springer.
- 15. Shilnikov L, Shilnikov A, Turaev D, Chua L (2001) Methods of Qualitative Theory in Nonlinear Dynamics - Part II. World Scientific Singapore.
- 16. Shilnikov L, Shilnikov A, Turaev D, Chua L (1998) Methods of Qualitative Theory in Nonlinear Dynamics - Part I. World Scientific Singapore.
- 17. Wolfram S (2002) A New Kind of Sciences. Wolfram Media Inc Champaign Illinois