Perturbation theory for nonequilibrium quantum fields

1993 ◽  
Vol 71 (5-6) ◽  
pp. 262-268 ◽  
Author(s):  
Ian D. Lawrie

Standard perturbation theory fails when applied to nonequilibrium processes. I explain why. To achieve sensible results, it is necessary to resum the absorptive parts of real-time self-energy corrections. Using the closed-time-path formalism, and in the context of scalar-field theory in an expanding universe, I show how a generalized renormalization technique can achieve this.

2007 ◽  
Vol 22 (12) ◽  
pp. 2173-2195 ◽  
Author(s):  
WEI FANG ◽  
H. Q. LU ◽  
Z. G. HUANG

The cosmological evolution in Nonlinear Born–Infeld (hereafter NLBI) scalar field theory with negative potentials was investigated. The cosmological solutions in some important evolutive epoches were obtained. The different evolutional behaviors between NLBI and linear (canonical) scalar field theory have been presented. A notable characteristic is that NLBI scalar field behaves as ordinary matter nearly the singularity while the linear scalar field behaves as "stiff" matter. We find that in order to accommodate current observational accelerating expanding universe the value of potential parameters |m| and |V0| must have an upper bound. We compare different cosmological evolutions for different potential parameters m, V0.


2001 ◽  
Vol 16 (supp01c) ◽  
pp. 1277-1280 ◽  
Author(s):  
Michael Strickland

I present a method for self-consistently including the effects of screening in finite-temperature field theory calculations. The method reproduces the perturbative limit in the weak-coupling limit and for intermediate couplings this method has much better convergence than standard perturbation theory. The method relies on a reorganization of perturbation theory accomplished by shifting the expansion point used to calculate quantum loop corrections. I will present results from a three-loop calculation within this formalism for scalar λϕ4.


1999 ◽  
Vol 14 (04) ◽  
pp. 257-266
Author(s):  
KRISHNENDU MUKHERJEE

We investigate the two-loop gap equation for the thermal mass of hot massless g2ϕ4 theory and find that the gap equation itself has a nonzero finite imaginary part. This implies that it is not possible to find the real thermal mass as a solution of the gap equation beyond g2 order in perturbation theory. We have solved the gap equation and obtained the real and imaginary parts of the thermal mass which are correct up to g4 order in perturbation theory.


1993 ◽  
Vol 08 (10) ◽  
pp. 1729-1753 ◽  
Author(s):  
ASIDA NAOKI

Calculational algorithm for thermal reaction probabilities including fermions is obtained. For this purpose, we faithfully follow the method of statistical mechanics, that is, taking explicitly the statistical average of the quantity under consideration. Our result is formulated in terms of Feynman rules of real time thermal field theory constructed on a specific time path. It is shown that the effect of the thermal vacuum bubble is of vital importance for analyzing diagrams with generalized self-energy parts.


2007 ◽  
Vol 85 (6) ◽  
pp. 671-677
Author(s):  
T Fugleberg ◽  
M E Carrington

In this paper, we discuss a Mathematica program that we have written that calculates the integrand for amplitudes in the closed-time-path formulation of real-time finite-temperature field theory. The program is designed to be used by someone with no previous experience with Mathematica. It performs contractions over tensor indices that appear in real-time finite-temperature field theory and gives the result in the 1-2, Keldysh or R/A basis. As an illustration of this program, we discuss the calculation of all 3-point ward identities in finite-temperature quantum electrodynamics with full vertices. PACS Nos.: 11.10.Wx,11.15.-q


2021 ◽  
Vol 2021 (06) ◽  
pp. 035
Author(s):  
Elena Kozlikin ◽  
Robert Lilow ◽  
Felix Fabis ◽  
Matthias Bartelmann

2007 ◽  
Vol 784 (1-4) ◽  
pp. 376-406 ◽  
Author(s):  
Jean-Paul Blaizot ◽  
Andreas Ipp ◽  
Ramón Méndez-Galain ◽  
Nicolás Wschebor

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