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Lattice QCD calculation of the $\pi^0$-pole contribution to the hadronic light-by-light scattering in the anomalous magnetic moment of the muon
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abstract
We develop a method to compute the pion transition form factor directly at arbitrary space-like photon momenta and use it to determine the $\pi^0$-pole contribution to the hadronic light-by-light scattering in the anomalous magnetic moment of the muon. The calculation is performed using eight gauge ensembles generated with 2+1 flavor domain wall fermions, incorporating multiple pion masses, lattice spacings, and volumes. By introducing a pion structure function and performing a Gegenbauer expansion, we demonstrate that about 98\% of the $\pi^0$-pole contribution can be extracted in a model-independent manner, thereby ensuring that systematic effects are well controlled. After applying finite-volume corrections, as well as performing chiral and continuum extrapolations, we obtain the final result for the $\pi^0$-pole contribution to the hadronic light-by-light scattering in the muon's anomalous magnetic moment, $a_{\mu}^{\pi^0\mathrm{-pole}}=61.2(1.7)\times 10^{-11}$, and the $\pi^0$ decay width, $\Gamma_{\pi^0\to \gamma\gamma}=7.60(27)$ eV.
Forward citations
Cited by 3 Pith papers
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Hadronic vacuum polarization for the muon $g-2$ from lattice QCD: Long-distance and full light-quark connected contribution
The light-quark connected hadronic vacuum polarization contribution to muon g-2 is determined to 0.69% precision, 655.2(4.5) x 10^-10, from lattice QCD.
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Pion Transition Form Factor in Lattice QCD
The disconnected quark-loop contribution to the pion transition form factor has the same sign as the connected contribution, at roughly 1% of its size, as calculated on one N_f=2+1 clover ensemble.
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Field-theoretical approach to neutral pion contribution to muon $g-2$
The neutral pion contribution to muon g-2 should contain only the on-shell pole term, with no principal-value part, because off-shell pions are not well-defined states in QCD.
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