$\mathcal{N}=4$ supersymmetric Yang-Mills thermodynamics from effective field theory

Abstract

The free energy density of $\mathcal{N}=4$ supersymmetric Yang-Mills theory in four space-time dimensions is derived through second order in the 't Hooft coupling $\lambda$ at finite temperature using effective-field theory methods. The contributions to the free energy density at this order come from the hard scale $T$ and the soft scale $\sqrt{\lambda }T$. The effects of the scale $T$ are encoded in the coefficients of an effective three-dimensional field theory that is obtained by dimensional reduction at finite temperature. The effects of the electric scale $\sqrt{\lambda }T$ are taken into account by perturbative calculations in the effective theory.

12 pages, 9 figures; v2 - minor typos fixes; published version

References in corpus (4)

• Phase Diagram of N=4 Super-Yang-Mills Theory with R-Symmetry Chemical Potentials
• On supersymmetry at finite temperature
• Two-loop HTL-resummed thermodynamics for N=4 supersymmetric Yang-Mills theory
• $\mathcal{N}=4$ supersymmetric Yang-Mills thermodynamics to order ${\lambda }^2$

Cited by in corpus (4)

• 50 Years of Quantum Chromodynamics
• Hard Thermal Loop -- theory and applications
• Constrained Padé Ensembles for Thermal N=4 SYM: Quantified Uncertainties and Next-Order Predictions
• Scheme dependence of two-loop HTLpt-resummed ${\text{SYM}}_{4,4}$ thermodynamics