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Nonrenormalizability of the classical statistical approximation

2014/02/07 by Thomas Epelbaum, François Gelis, Francois Gelis +1
Mathematics · Physics and Astronomy · #Advanced Thermodynamics and Statistical Mechanics #Applied mathematics #Approximation error #Approximation theory #Born–Huang approximation #Field (mathematics) #High frequency approximation #High-Energy Particle Collisions Research #Linear approximation #Mathematical analysis #Mathematics #Muffin-tin approximation #Physics #Quantum #Quantum field theory #Quantum mechanics #Scattering #Scheme (mathematics) #Spouge's approximation #Statistical Mechanics and Entropy #Statistical physics #hep-ph #hep-th #nucl-th

paper · pdf · doi:10.1103/physrevd.90.065029

published as Phys. Rev. D 90, 065029 (2014) · 31 pages, 29 figures

arxiv created 2014/02/07 · openalex publication_date 2014/09/23 · arxiv updated 2014/10/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

In this paper, we discuss questions related to the renormalizability of the classical statistical approximation, an approximation scheme that has been used recently in several studies of out-of-equilibrium problems in quantum field theory. Although the ultraviolet power counting in this approximation scheme is identical to that of the unapproximated quantum field theory, this approximation is not renormalizable. The leading cause of this nonrenormalizability is the breakdown of Weinberg's theorem in this approximation. We also discuss some practical implications of this negative result for simulations that employ this approximation scheme, and we speculate about a possible modification of the classical statistical approximation in order to systematically subtract the leading residual divergences.

Citations