η→γ*γ* transition form factor and the hadronic light-by-light η

We calculate the double-virtual $\ensuremath{\eta}\ensuremath{\rightarrow}{\ensuremath{\gamma}}^{*}{\ensuremath{\gamma}}^{*}$ transition form factor ${\mathcal{F}}_{\ensuremath{\eta}\ensuremath{\rightarrow}{\ensuremath{\gamma}}^{*}{\ensuremath{\gamma}}^{*}}({q}_{1}^{2},{q}_{2}^{2})$ from first principles using a lattice QCD simulation with ${N}_{f}=2+1+1$ quark flavors at the physical pion mass and at one lattice spacing and volume. The kinematic range covered by our calculation is complementary to the one accessible from experiment and is relevant for the $\ensuremath{\eta}$-pole contribution to the hadronic light-by-light scattering in the anomalous magnetic moment ${a}_{\ensuremath{\mu}}=(g\ensuremath{-}2)/2$ of the muon. From the form factor calculation we extract the partial decay width $\mathrm{\ensuremath{\Gamma}}(\ensuremath{\eta}\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\gamma})=338(87{)}_{\mathrm{stat}}(17{)}_{\mathrm{syst}}\text{ }\text{ }\mathrm{eV}$ and the slope parameter ${b}_{\ensuremath{\eta}}=1.34(28{)}_{\mathrm{stat}}(14{)}_{\mathrm{syst}}\text{ }\text{ }{\mathrm{GeV}}^{\ensuremath{-}2}$. For the $\ensuremath{\eta}$-pole contribution to ${a}_{\ensuremath{\mu}}$ we obtain ${a}_{\ensuremath{\mu}}^{\ensuremath{\eta}\text{-pole}}=13.8(5.2{)}_{\mathrm{stat}}(1.5{)}_{\mathrm{syst}}\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}$.