Isospin symmetry breaking and gluon anomaly
A. A. Osipov
TL;DR
This work analyzes electromagnetic isospin breaking in the pseudoscalar meson nonet within the framework of large-$N_c$ chiral perturbation theory, explicitly including singlet–octet mixing and the $U(1)_A$ gluon anomaly. By organizing the theory in an $oldsymbol{ ext{O}}(oldsymbol{oldsymbol{ au}})$ expansion with $ ext{O}(m_q)= ext{O}(p^2)= ext{O}(1/N_c)= ext{O}(oldsymbol{ au})$ and $ ext{O}(e^2)= ext{O}(oldsymbol{ au})$, the authors compute electromagnetic self-energies, masses, decay constants, and mixing angles for neutral pseudoscalars at next-to-leading order. A key finding is that the $U(1)_A$ anomaly enhances EM contributions to $oldsymbol{π^0}$–$oldsymbol{η}$ and $oldsymbol{π^0}$–$oldsymbol{η’}$ mixing, driving isospin restoration in the neutral-meson spectrum at NLO, while the EM effect on the $oldsymbol{η}$–$oldsymbol{η’}$ mixing angle remains small (about 3%). The analysis yields a two-angle description for the $oldsymbol{η}$–$oldsymbol{η’}$ system with $oldsymbol{ϑ_8} oughly -21^ ext{o}$ and $oldsymbol{ϑ_0} oughly -2^ ext{o}$, and a near-Gross–Treiman–Wilczek value for $oldsymbol{π^0}$–$oldsymbol{η}$ mixing, demonstrating a subtle interplay between electromagnetic, quark-mass, and anomaly effects in isospin violation.
Abstract
The contribution of the electromagnetic interaction to the self-energy of pseudo-Goldstone bosons, as well as to the mixing angles and weak decay constants, is calculated in the first nonleading order in the simultaneous expansion in powers of $1/N_c$, momenta and quark masses. Particular attention is paid to the isospin symmetry breaking which is generated by means of $η$ and $η'$ admixtures to the pion. It is shown that the gluon anomaly enhances the electromagnetic contribution to the $π^0$-$η$ and $π^0$-$η'$ mixing angles, which facilitates the restoration of isospin symmetry in the spectrum of pseudo-Goldstone states at next-to-leading order. The contribution of the electromagnetic interaction to the $η$-$η'$ mixing angle is shown to be only about 3\%.
