Abstract
We have computed the hadronic light-by-light (LbL) contribution to the muon
anomalous magnetic moment \$a\_\mu\$ in the frame of Chiral Perturbation Theory
with the inclusion of the lightest resonance multiplets as dynamical fields
(R\$\chi\$T). It is essential to give a more accurate prediction of this hadronic
contribution due to the future projects of J-Parc and FNAL on reducing the
uncertainty in this observable. We, therefore, computed the pseudoscalar
transition form factor and proposed the measurement of the
\$e^+e^-\to\mu^+\mu^-\pi^0\$ cross section and dimuon invariant mass spectrum to
determine more accurately its parameters. Then, we evaluated the pion exchange
contribution to \$a\_\mu\$, obtaining \$(6.66\pm0.21)\cdot10^-10\$. By comparing
the pion exchange contribution and the pion-pole approximation to the
corresponding transition form factor (\$\pi\$TFF) we recalled that the latter
underestimates the complete \$\pi\$TFF by (15-20)\%. Then, we obtained the
\$\eta^('^)\$ TFF, obtaining a total contribution of the lightest pseudoscalar
exchanges of \$(10.47\pm0.54)\cdot10^-10\$, in agreement with previous results
and with smaller error.
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