2000/07/12 by Ian D. Lawrie, I. D. Lawrie, D. B. McKernan · 4 citations
Physics and Astronomy · #Advanced Thermodynamics and Statistical Mechanics #Mathematical physics #Non-equilibrium thermodynamics #Perturbation theory (quantum mechanics) #Physics #Physics of Superconductivity and Magnetism #Quantum many-body systems #Quantum mechanics #Quasiparticle #Thermal equilibrium #gr-qc #hep-ph #hep-th
paper · pdf · doi:10.1103/physrevd.62.105032
published in Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 62(10) (American Physical Society) · 16 pages; no figures; submitted to Phys. Rev. D
arxiv created 2000/07/12 · openalex publication_date 2000/10/26 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
A partial resummation of perturbation theory is described for field theories containing spin-(1)/(2) particles in states that may be far from thermal equilibrium. This allows the nonequilibrium state to be characterized in terms of quasiparticles that approximate its true elementary excitations. In particular, the quasiparticles have dispersion relations that differ from those of free particles, finite thermal widths and occupation numbers which, in contrast with those of standard perturbation theory, evolve with the changing nonequilibrium environment. A description of this kind is essential for estimating the evolution of the system over extended periods of time. In contrast with the corresponding description of scalar particles, the structure of nonequilibrium fermion propagators exhibits features which have no counterpart in the equilibrium theory.