Controlled nonperturbative dynamics of quantum fields out-of-equilibrium
By J. Berges. 2001
195 citations recorded by the source corpus.
Abstract We compute the nonequilibrium real-time evolution of an O ( N )-symmetric scalar quantum field theory from a systematic 1/ N expansion of the 2PI effective action to next-to-leading order, which includes scattering and memory effects. In contrast to the standard 1/ N expansion of the 1PI effective action, the next-to-leading-order expansion in presence of a possible expectation value for the composite operator leads to a bounded-time evolution where the truncation error may be controlled by higher powers in 1/ N . We present a detailed comparison with the leading-order results and determine the range of validity of standard mean-field-type approximations. We investigate “quench” and “tsunami” initial conditions frequently used to mimic idealized far-from-equilibrium pion dynamics in the context of heavy-ion collisions. For spatially homogeneous initial conditions, we find three generic regimes, characterized by an early-time exponential damping, a parametrically slow (power-law) behavior at intermediate times, and a late-time exponential approach to thermal equilibrium. The different time scales are obtained from a numerical solution of the time-reversal invariant equations in 1+1 dimensions without further approximations. We discuss in detail the out-of-equilibrium behavior of the nontrivial n -point correlation functions as well as the evolution of a particle number distribution and inverse slope parameter.
Subfields: Astronomy and Astrophysics, Atomic and Molecular Physics, and Optics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/b021accc9dbdaa253553802d0681905d61f035f8
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Citations in the corpus
- TRANSPORT EQUATIONS FOR CHIRAL FERMIONS TO ORDER ħ AND ELECTROWEAK BARYOGENESIS (2004, background): “One can in fact study the quantum dynamics of scalar fields also in the strongly coupled regime by making use of the 1/N expansion, where N denotes the number of scalar field components [22, 23, 24].”