LinkingU(2)×U(2)toO(4)model via decoupling

Abstract

The nature of chiral phase transition of massless two flavor QCD depends on the fate of flavor singlet axial symmetry ${U}_{A}(1)$ at the critical temperature (${T}_{c}$). Assuming that a finite ${U}_{A}(1)$ breaking remains at ${T}_{c}$, the corresponding three dimensional effective theory is composed of four massless and four massive scalar fields. We study the renormalization group flow of the effective theory in the $\ensuremath{\epsilon}$-expansion, using a mass dependent renormalization scheme, and determine the region of the attractive basin flowing into the $O(4)$ fixed point with a focus on its dependence on the size of the ${U}_{A}(1)$ breaking. The result is discussed from a perspective of the decoupling of massive fields. It is pointed out that, although the effective theory inside the attractive basin eventually reaches the $O(4)$ fixed point, the approaching rate, one of the universal exponents, is different from that of the standard $O(4)$ model. We present the reason for this peculiarity, and propose a novel possibility for chiral phase transition in two-flavor QCD.