Kinked Entropy and Discontinuous Microcanonical Spontaneous Symmetry Breaking
arXiv:1901.00125 · doi:10.1103/PhysRevLett.122.160601
Abstract
Spontaneous symmetry breaking (SSB) in statistical physics is a macroscopic collective phenomenon. For the paradigmatic Q-state Potts model it means a transition from the disordered color-symmetric phase to an ordered phase in which one color dominates. Existing mean field theories imply that SSB in the microcanonical statistical ensemble (with energy being the control parameter) should be a continuous process. Here we study microcanonical SSB on the random-graph Potts model, and discover that the entropy is a kinked function of energy. This kink leads to a discontinuous phase transition at certain energy density value, characterized by a jump in the density of the dominant color and a jump in the microcanonical temperature. This discontinuous SSB in random graphs is confirmed by microcanonical Monte Carlo simulations, and it is also observed in bond-diluted finite-size lattice systems.
16 pages, extensively revised and improved
References in corpus (10)
- Statistical mechanics and dynamics of solvable models with long-range interactions
- Equivalence and nonequivalence of ensembles: Thermodynamic, macrostate, and measure levels
- Microcanonical Approach to the Simulation of First-Order Phase Transitions
- Phase Transitions of Ferromagnetic Potts Models on the Simple Cubic Lattice
- Statistical Mechanics of systems with long range interactions
- A simple model for multiple-choice collective decision making
- Universal Critical Wrapping Probabilities in the Canonical Ensemble
- Ground-state configuration space heterogeneity of random finite-connectivity spin glasses and random constraint satisfaction problems
- Ensemble Inequivalence in the Spherical Spin Glass Model with Nonlinear Interactions
- Scaling in the vicinity of the four-state Potts fixed point