Field theory of birhythmicity

Nonequilibrium dynamics are present in many aspects of our lives, ranging from microscopic physical systems to the functioning of the brain. What characterizes stochastic models of nonequilibrium processes is the breaking of the fluctuation-dissipation relations as well as the existence of nonstatic stable states, or phases. A prototypical example is a dynamical phase characterized by a limit cycle-the order parameter of finite magnitude rotating or oscillating at a fixed frequency. Consequently, birhythmicity, where two stable limit cycles coexist, is a natural extension of the simpler single limit cycle phase. Both the abundance of real systems exhibiting such states and their relevance for building our understanding of nonequilibrium phases and phase transitions are strong motivations to build and study models of such behavior. Field-theoretic tools can be used to provide insights into either phase and the transition between them. In this work, we explore a simple linear model of a single limit cycle phase with phase-amplitude coupling. We demonstrate how such nonequilibrium coupling affects the fluctuation spectrum of the theory. We then extend this model to include a continuous transition to a two-cycle phase. We give various results, such as the appearance of a critical exceptional point, the destruction of the transition, the enhancement of noise for the phase, and the presence of Kardar-Parisi-Zhang(KPZ) dynamics. Finally, we qualitatively demonstrate these results with numerics and discuss future directions.