Free energy on the sphere for non-abelian gauge theories

We compute the S-d partition function of the fixed point of non-abelian gauge theories in continuous d, using the e-expansion around d = 4. We illustrate in detail the technical aspects of the calculation, including all the factors arising from the gauge-fixing procedure, and the method to deal with the zero-modes of the ghosts. We obtain the result up to NLO, i.e. including two-loop vacuum diagrams. Depending on the sign of the one-loop beta function, there is a fixed point with real gauge coupling in d > 4 or d < 4. In the first case we extrapolate to d = 5 to test a recently proposed construction of the UV fixed point of 5d SU(2) Yang-Mills via a susy-breaking deformation of the E-1 SCFT. We find that the F theorem allows the proposed RG flow. In the second case we extrapolate to d = 3 to test whether QCD(3) with gauge group SU(n(c)) and n(f) fundamental matter fields flows to a CFT or to a symmetry-breaking case. We find that within the regime with a real gauge coupling near d = 4 the CFT phase is always favored. For lower values of n(f) we compare the average of F between the two complex fixed points with its value at the symmetry-breaking phase to give an upper bound of the critical value n*(f) below which the symmetry-breaking phase takes over.

Automated summary

This paper computes the S-d partition function of the fixed point of non-abelian gauge theories in continuous d, using the e-expansion around d = 4. The technical aspects of the calculation, including gauge-fixing procedure and handling of ghost zero-modes, are detailed. The result up to NLO, including two-loop vacuum diagrams, is obtained. The study examines the UV fixed point of 5d SU(2) Yang-Mills via a susy-breaking deformation of the E-1 SCFT and the behavior of QCD(3) with gauge group SU(n(c)) and n(f) fundamental matter fields.