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Hadronic light-by-light corrections to the muon<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>g</mml:mi><mml:mi>โˆ’</mml:mi><mml:mn>2</mml:mn><mml:mo>:</mml:mo></mml:math>The pion-pole contribution

Hadronic light-by-light corrections to the muon<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>g</mml:mi><mml:mi>โˆ’</mml:mi><mml:mn>2</mml:mn><mml:mo>:</mml:mo></mml:math>The pion-pole contribution

The correction to the muon anomalous magnetic moment from the pion-pole contribution to the hadronic light-by-light scattering is considered using a description of the ${\ensuremath{\pi}}^{0}\ensuremath{-}{\ensuremath{\gamma}}^{*}\ensuremath{-}{\ensuremath{\gamma}}^{*}$ transition form factor based on the large-${N}_{C}$ and short-distance properties of QCD. The resulting two-loop integrals are treated by first performing the angular integration analytically, โ€ฆ