2013
DOI: 10.1007/s10955-013-0756-2
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A Curie-Weiss Model with Dissipation

Abstract: We consider stochastic dynamics for a spin system with mean field interaction, in which the interaction potential is subject to noisy and dissipative stochastic evolution. We show that, in the thermodynamic limit and at sufficiently low temperature, the magnetization of the system has a time periodic behavior, despite of the fact that no periodic force is applied

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Cited by 24 publications
(43 citation statements)
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“…With this observation, we follow a long tradition, see e.g. [33,34] in the framework of nonlinear diffusion processes, or Dai Pra, Fischer and Regoli (2015) [12] and Collet, Dai Pra and Formentin (2015) [9].…”
Section: Oscillationsmentioning
confidence: 86%
See 1 more Smart Citation
“…With this observation, we follow a long tradition, see e.g. [33,34] in the framework of nonlinear diffusion processes, or Dai Pra, Fischer and Regoli (2015) [12] and Collet, Dai Pra and Formentin (2015) [9].…”
Section: Oscillationsmentioning
confidence: 86%
“…This study follows a long tradition, starting probably with [33,34] in the framework of nonlinear diffusion processes, or Dai Pra, Fischer and Regoli (2015) [12], Collet, Dai Pra and Formentin (2015) [9] and Collet, Formentin and Tovazzi (2016) [10]. In all these papers, rhythmic behavior arises in the mean field limit as a consequence of the nonlinear "Mc-Kean-Vlasov"-type dynamics of the limit process.…”
Section: Introductionmentioning
confidence: 99%
“…Example. If we set Γ (z) = 1 + tanh(z), the analysis of the phase diagram done in [11,Sect. 3] is recovered.…”
Section: Under the Assumptionmentioning
confidence: 99%
“…The process ζ n is the effective potential felt by the i-th particle and it is damped in time according to the equation dζ n = −αζ n dt + βdm n (α, β > 0), where m n = n −1 n i=1 σ i is the empirical average of the spins. Compared to the original version of the dissipative Curie-Weiss model [11], we do not have any external noise in the evolution of ζ n (as in [14]); on the other hand, we work with arbitrary transition rates rather than sticking on the case Γ (x) = 1 + tanh(x). Depending on the choice of the function Γ , the phase structure of the infinite volume system may become very rich.…”
Section: Introductionmentioning
confidence: 99%
“…One of the goals of the mathematical theory in this field is to understand which types of microscopic interactions and mechanisms can lead to or enhance the above self-organization. Among others, we cite noise ( [10], [20], [22]), dissipation in the interaction potential ( [1], [6], [7], [9]), delay in the transmission of information and/or frustration in the interaction network ( [8], [12], [21]). In particular, in [12] the authors consider non-Markovian dynamics, studying systems of interacting nonlinear Hawkes processes for modeling neurons.…”
Section: Introductionmentioning
confidence: 99%