The role of U(1)A symmetry breaking in the QCD corrections to the pion mass difference

The charged and neutral pion mass difference can be attributed to both the QED and QCD contributions. The current quark mass difference (Δm) is the source of the QCD contribution. Here, in a two flavour non-local NJL model, we try to estimate the QCD contribution. Interestingly, we find that the strength of the U(1)A symmetry breaking parameter c plays a crucial role in obtaining the pion mass difference while intertwined with the current quark mass difference. To obtain the QCD contribution for the pion mass difference, we scan the parameter space in {∆m, c}, and by comparing this with the existing results, we constrained the parameter space. Further, using a fitted value of c, we determine the allowed range for the Δm in the model. The model estimated Δm ranges enable us to extract the chiral perturbation theory low energy constant, l 7 and verify the dependence of the pion mass difference on Δm. We also find out its dependence on c — it increases with the decreasing value of c, i.e., toward an axial anomaly restored phase.