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We have studied the $Ptogamma^stargamma^star$ form factor in Resonance Chiral Theory, with $P = pi^0etaeta$, to compute the contribution of the pseudoscalar pole to the hadronic light-by-light piece of the anomalous magnetic moment of the muon. In this work we allow the leading $U(3)$ chiral symmetry breaking terms, obtaining the most general expression for the form factor up to $mathcal{O}(m_P^2)$. The parameters of the Effective Field Theory are obtained by means of short distance constraints on the form factor and matching with the expected behavior from QCD. Those parameters that cannot be fixed in this way are fitted to experimental determinations of the form factor within the spacelike region. Chiral symmetry relations among the transition form factors for $pi^0,eta$ and $eta$ allow for a simultaneous fit to experimental data for the three mesons. This shows an inconsistency between the BaBar $pi^0$ data and the rest of the experimental inputs. Thus, we find a total pseudoscalar pole contribution of $a_mu^{P,HLbL}=(8.47pm 0.16)cdot 10^{-10}$ for our best fit (that neglecting the BaBar $pi^0$ data). Also, a preliminary rough estimate of the impact of NLO in $1/N_C$ corrections and higher vector multiplets (asym) enlarges the uncertainty up to $a_mu^{P,HLbL}=(8.47pm 0.16_{rm stat}pm 0.09_{N_C}{}^{+0.5}_{-0.0_{rm asym}})10^{-10}$.
In this work we study the axial contributions to the hadronic light-by-light piece of the muon anomalous magnetic moment using the framework of resonance chiral theory. As a result, we obtain $a_{mu}^{textrm{HLbL};A} = left(0.8^{+3.5}_{-0.1}right)cdo
The evaluation of the numerically dominant pseudoscalar-pole contribution to hadronic light-by-light scattering in the muon g-2 involves the pseudoscalar-photon transition form factor F_{P gamma^* gamma^*}(-Q_1^2, -Q_2^2) with P = pi^0, eta, eta^prim
The evaluation of the numerically dominant pseudoscalar-pole contribution to hadronic light-by-light scattering in the muon g-2 involves the pseudoscalar-photon transition form factor F_{P gamma^* gamma^*}(-Q_1^2, -Q_2^2) with P = pi^0, eta, eta^prim
The $pi^0$ pole constitutes the lowest-lying singularity of the hadronic light-by-light (HLbL) tensor, and thus provides the leading contribution in a dispersive approach to HLbL scattering in the anomalous magnetic moment of the muon $(g-2)_mu$. It
Using an effective sigma/f_0(500) resonance, which describes the pipi-->pipi and gammagamma-->pipi scattering data, we evaluate its contribution and the ones of the other scalar mesons to the the hadronic light-by-light (HLbL) scattering component of