Quasi-particle re-summation and integral gap equation in thermal field theory

TL;DR

This paper introduces a novel quasi-particle re-summation method for finite-temperature quantum field theories, deriving an integral gap equation that generalizes thermodynamic concepts across various dimensions and models.

Contribution

It develops a new approach to finite-temperature quantum field theory using integral equations for quasi-particle energies, extending thermodynamic Bethe ansatz and defining a thermal c-function in arbitrary dimensions.

Findings

Reduces to thermodynamic Bethe ansatz in 2D integrable theories

Defines a thermal c-function applicable in any dimension

Suggests a classification scheme for rational theories using polylogarithmic ladders

Abstract

A new approach to quantum field theory at finite temperature and density in arbitrary space-time dimension D is developed. We focus mainly on relativistic theories, but the approach applies to non-relativistic ones as well. In this quasi-particle re-summation, the free energy takes the free-field form but with the one-particle energy $\omega (\vec{k})$ replaced by $\vep (\vec{k})$, the latter satisfying a temperature-dependent integral equation with kernel related to a zero temperature form-factor of the trace of stress-energy tensor. For 2D integrable theories the approach reduces to the thermodynamic Bethe ansatz. For relativistic theories, a thermal c-function $C_{\rm qs} (T)$ is defined for any $D$ based on the coefficient of the black body radiation formula. Thermodynamical constraints on it's flow are presented, showing that it can violate a ``c-theorem'' even in 2D. At a fixed point $C_{\rm qs}$ is a function of thermal gap parameters which generalizes Roger's dilogarithm to higher dimensions. This points to a strategy for classifying rational theories based on ``polylogarithmic ladders'' in mathematics, and many examples are worked out. An argument suggests that the 3D Ising model has $C_{\rm qs} = 7/8$. (In 3D a free fermion has $C_{\rm qs} = 3/4$.) Other applications are discussed, including the free energy of anyons in 2D and 3D, phase transitions with a chemical potential, and the equation of state for cosmological dark energy.