Relaxation of 2+1 dimensional classical O(2) symmetric scalar fields
arXiv:hep-ph/0011283 · doi:10.1016/S0370-2693(01)00443-9
Abstract
Real time thermalization and relaxation phenomena are studied in the low energy density phase of the 2+1 dimensional classical O(2) symmetric scalar theory by solving numerically its dynamics. The near-equilibrium decay rate of on-shell waves and the power law governing the large time asymptotics of the off-shell relaxation agree with the analytic results based on linear response theory. The realisation of the Mermin-Wagner theorem is also studied in the final equilibrium ensemble.
9 Latex pages, 3 figures, final version to appear in Phys. Lett. B
References in corpus (5)
- On Thermalization in Classical Scalar Field Theory
- Time evolution of correlation functions and thermalization
- Fate of the classical false vacuum
- Effective theory for the soft fluctuation modes in the spontaneously broken phase of the N-component scalar field theory
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- Turbulent Thermalization
- Low-cost fermions in classical field simulations
- The O(N) linear sigma model at finite temperature beyond the Hartree approximation
- Isotropization far from equilibrium
- Out of Equilibrium Non-perturbative Quantum Field Dynamics in Homogeneous External Fields
- Ising-like dynamical signatures and the end-point of the QCD transition line
- Expanding non homogeneous configurations of the model
- Time evolution in linear response: Boltzmann equations and beyond
- Out of equilibrium quantum field dynamics of an initial thermal state after a change in the external field