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Phase coexistence in a weakly stochastic reaction-diffusion system.

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We studied phase coexistence in a reaction-diffusion system without using a continuum model. The phase coexistence condition depends on hopping rates between vessels, with distinct potentials for high and low rates.

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Area of Science:

  • Chemical kinetics
  • Statistical mechanics
  • Non-equilibrium systems

Background:

  • Reaction-diffusion systems are fundamental to understanding pattern formation and complex behaviors in chemistry and biology.
  • Phase coexistence, where distinct chemical states coexist, is a key phenomenon in bistable systems.
  • Continuum approximations are often used but may obscure discrete effects in spatially extended systems.

Purpose of the Study:

  • To investigate phase coexistence in a weakly stochastic reaction-diffusion system without relying on a continuum description.
  • To derive a condition for phase coexistence in a system of (2N+1) diffusion-coupled vessels as N approaches infinity.
  • To analyze the dependence of phase coexistence on the rate of particle hopping between neighboring vessels.

Main Methods:

  • Development of a discrete model for a reaction-diffusion system with bistable kinetics.
  • Derivation of the phase coexistence condition in the thermodynamic limit (N→∞).
  • Analysis of the system's behavior in high- and low-hopping rate regimes.

Main Results:

  • A condition for phase coexistence was derived for the discrete reaction-diffusion system.
  • The phase coexistence condition was found to be dependent on the hopping rate between vessels.
  • Distinct potentials governing phase coexistence were identified for high- and low-hopping rate limits, derived from the single-vessel reaction kinetics.

Conclusions:

  • Phase coexistence in weakly stochastic reaction-diffusion systems can be understood without continuum approximations.
  • The hopping rate between discrete spatial locations plays a critical role in determining phase coexistence.
  • The derived potentials offer insights into the microscopic mechanisms underlying macroscopic phase separation.