Home

About

Advanced Search

Browse by Discipline

Scientific Societies

E-print Alerts

Add E-prints

E-print Network
FAQHELPSITE MAPCONTACT US


  Advanced Search  

 
Nuclear Physics B 587 (2000) 403418 www.elsevier.nl/locate/npe
 

Summary: Nuclear Physics B 587 (2000) 403­418
www.elsevier.nl/locate/npe
On thermalization in classical scalar field theory
Gert Aarts , Gian Franco Bonini, Christof Wetterich
Institut für theoretische Physik, Universität Heidelberg, Philosophenweg 16, 69120 Heidelberg, Germany
Received 29 March 2000; revised 21 May 2000; accepted 11 July 2000
Abstract
Thermalization of classical fields is investigated in a 4 scalar field theory in 1 + 1 dimensions,
discretized on a lattice. We numerically integrate the classical equations of motion using initial con-
ditions sampled from various nonequilibrium probability distributions. Time-dependent expectation
values of observables constructed from the canonical momentum are compared with thermal ones. It
is found that a closed system, evolving from one initial condition, thermalizes to high precision in the
thermodynamic limit, in a time-averaged sense. For ensembles consisting of many members with the
same energy, we find that expectation values become stationary -- and equal to the thermal values
-- in the limit of infinitely many members. Initial ensembles with a nonzero (noncanonical) spread
in the energy density or other conserved quantities evolve to noncanonical stationary ensembles. In
the case of a narrow spread, asymptotic values of primary observables are only mildly affected. In
contrast, fluctuations and connected correlation functions will differ substantially from the canonical
values. This raises doubts on the use of a straightforward expansion in terms of 1PI-vertex functions
to study thermalization. © 2000 Elsevier Science B.V. All rights reserved.

  

Source: Aarts, Gert - Department of Physics, University of Wales Swansea

 

Collections: Physics