Abstract

Discontinuous transitions have received considerable interest due to the uncovering that many phenomena such as catastrophic changes, epidemic outbreaks and synchronization present a behavior signed by abrupt (macroscopic) changes (instead of smooth ones) as a tuning parameter is changed. However, in different cases there are still scarce microscopic models reproducing such above trademarks. With these ideas in mind, we investigate the key ingredients underpinning the discontinuous transition in one of the simplest systems with up-down Z2 symmetry recently ascertained in [Phys. Rev. E 95, 042304 (2017)]. Such system, in the presence of an extra ingredient-the inertia- has its continuous transition being switched to a discontinuous one in complex networks. We scrutinize the role of three central ingredients: inertia, system degree, and the lattice topology. Our analysis has been carried out for regular lattices and random regular networks with different node degrees (interacting neighborhood) through mean-field theory (MFT) treatment and numerical simulations. Our findings reveal that not only the inertia but also the connectivity constitute essential elements for shifting the phase transition. Astoundingly, they also manifest in low-dimensional regular topologies, exposing a scaling behavior entirely different than those from the complex networks case. Therefore, our findings put on firmer bases the essential issues for the manifestation of discontinuous transitions in such relevant class of systems with Z2 symmetry.

Highlights

  • Spontaneous breaking symmetry manifests in a countless sort of systems besides the classical ferromagneticparamagnetic phase transition[1,2]

  • mean-field theory (MFT) insights us that large θ and k (k ≥ 6) are core ingredients for the appearance of a discontinuous phase transition

  • A discontinuous phase transition in the standard majority vote model has been recently discovered in the presence of an extra ingredient: the inertia

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Summary

Introduction

Spontaneous breaking symmetry manifests in a countless sort of systems besides the classical ferromagneticparamagnetic phase transition[1,2]. Systems with Z2 (“up-down”) symmetry constitute ubiquitous models of spontaneous breaking symmetry, and their phase transitions and universality classes have been an active topic of research during the last decades[1,2,6]. Several transitions between the distinct regimes do not follow smooth behaviors[7,8,9], but instead, they manifest through abrupt shifts. These discontinuous (nonequilibrium) transitions have received much less attention than the critical transitions and a complete understanding of their essential aspects is still lacking.

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