2020
DOI: 10.1016/j.chaos.2020.109618
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Phase space classification of an Ising cellular automaton: The Q2R model

Abstract: An exact characterization of the different dynamical behavior that exhibit the space phase of a reversible and conservative cellular automaton, the so called Q2R model, is shown in this paper. Q2R is a cellular automaton which is a dynamical variation of the Ising model in statistical physics and whose space of configurations grows exponentially with the system size. As a consequence of the intrinsic reversibility of the model, the phase space is composed only by configurations that belong to a fixed point or … Show more

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Cited by 6 publications
(5 citation statements)
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“…This system has energy E = −9, and under the rule section 2.2, the dynamics is shown in figure 4. First, this system has period T = 4, and due to theorem 4.10 [16], is classified as an asymmetric cycle, e.i., it has always different configurations.…”
Section: An Exact Phase Space Classification: System Size L =mentioning
confidence: 99%
See 1 more Smart Citation
“…This system has energy E = −9, and under the rule section 2.2, the dynamics is shown in figure 4. First, this system has period T = 4, and due to theorem 4.10 [16], is classified as an asymmetric cycle, e.i., it has always different configurations.…”
Section: An Exact Phase Space Classification: System Size L =mentioning
confidence: 99%
“…Due to the reversibility of this model, Hermann et al [13] demonstrated that the model dynamics can have periods of 'infinite' length on lattices of 'infinite' size. In this context, Montalva et al [16] classified the entire space of 2 32 ≈ 4.3 × 10 9 configurations by identifying all the fixed points and the orbits for each energy's value. Moreover, they presented a theorem that classifies the different types of cycles: symmetric and asymmetric.…”
Section: Introductionmentioning
confidence: 99%
“…In this study, we assume a second-order neighborhood system, that is, ∆ = 8, defining the Moore neighborhood. In each site s i we observe a random variable x i that assume values in {−1, +1}, representing the spin of a particle [28]. A realization X = (x k ) k∈S is an assignment of a spin value to each s i , for i = 1, 2, ..., n. For any pair of adjacent sites s i , s j ∈ S there is an interaction J ij .…”
Section: The Ising Modelmentioning
confidence: 99%
“…Several studies have carried out concerning the Q2R [1,5,6,7,8,9,10,11,12]. Remarkably, the Q2R dynamic preserves an Ising-like energy [5], appealing the analogy with the continuous dynamics of Hamiltonian systems.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, in an attempt to establish general mathematical properties, a full characterization and combinatorial results of the attractors associated to the Q2R model were proposed in [12]. In tune with this mathematical approach, in this paper we tackle an analytical study of the dynamics and complexity of Q2R.…”
Section: Introductionmentioning
confidence: 99%