Thermal field theory at next-to-leading order in the hard thermal loop expansion

A. Mirza and M. E. Carrington
Phys. Rev. D 87, 065008 – Published 12 March 2013

Abstract

In this paper we study the hard-thermal-loop effective theory at next-to-leading order. Standard power counting predicts that a large number of diagrams, including 2-loop diagrams, may need to be calculated. In all of the calculations that have been done however, with the exception of the photon self-energy, the full next-to-leading order contribution can be obtained by calculating only soft 1-loop diagrams with effective lines and vertices. It is of interest to know if the photon self-energy is the only exception to this rule, or if there are others, and which ones. In this paper we perform a refined power-counting analysis using real-time finite temperature field theory which is particularly well suited to the task. We show that the standard power-counting rules obtained from the imaginary time formalism usually overestimate the size of the 2-loop diagrams. We argue that the only exceptions to the rule that the 1-loop soft diagrams give the next-to-leading order contribution are 2n-photon vertices.

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  • Received 7 December 2012

DOI:https://doi.org/10.1103/PhysRevD.87.065008

© 2013 American Physical Society

Authors & Affiliations

A. Mirza* and M. E. Carrington

  • Department of Physics, Brandon University, Brandon, Manitoba R7A 6A9, Canada and Winnipeg Institute for Theoretical Physics, Winnipeg, Manitoba, Canada

  • *mirzaalx@gmail.com
  • carrington@brandonu.ca

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Vol. 87, Iss. 6 — 15 March 2013

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