Pressure to order $g^8*log(g)$ in $\phi^4$-theory at weak coupling
Jens O. Andersen, Lars Kyllingstad, and Lars E. Leganger

TL;DR
This paper computes the pressure of massless $^4$-theory up to order $g^8 \log(g)$ at weak coupling, employing effective field theory and dimensional reduction to separate and evaluate contributions from different momentum scales.
Contribution
It advances the calculation of thermodynamic pressure in $^4$-theory to higher order, including $g^8 \log(g)$, using novel multi-loop sum-integrals and renormalization group techniques.
Findings
Pressure calculated up to order $g^8 \\log(g)$ at weak coupling.
Effective field theory separates hard and soft contributions.
Results improve understanding of perturbative series convergence.
Abstract
We calculate the pressure of massless -theory to order at weak coupling. The contributions to the pressure arise from the hard momentum scale of order and the soft momentum scale of order . Effective field theory methods and dimensional reduction are used to separate the contributions from the two momentum scales: The hard contribution can be calculated as a power series in using naive perturbation theory with bare propagators. The soft contribution can be calculated using an effective theory in three dimensions, whose coefficients are power series in . This contribution is a power series in starting at order . The calculation of the hard part to order involves a complicated four-loop sum-integral that was recently calculated by Gynther, Laine, Schr\"oder, Torrero, and Vuorinen. The calculation of the soft part requires calculating…
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