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The charm-quark contribution to light-by-light scattering in the muon [Formula: see text] from lattice QCD
We compute the hadronic light-by-light scattering contribution to the muon [Formula: see text] from the charm quark using lattice QCD. The calculation is performed on ensembles generated with dynamical (u, d, s) quarks at the SU(3)[Formula: see text] symmetric point with degenerate pion and kaon mas...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Springer Berlin Heidelberg
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9345843/ https://www.ncbi.nlm.nih.gov/pubmed/35937708 http://dx.doi.org/10.1140/epjc/s10052-022-10589-2 |
Sumario: | We compute the hadronic light-by-light scattering contribution to the muon [Formula: see text] from the charm quark using lattice QCD. The calculation is performed on ensembles generated with dynamical (u, d, s) quarks at the SU(3)[Formula: see text] symmetric point with degenerate pion and kaon masses of around 415 MeV. It includes the connected charm contribution, as well as the leading disconnected Wick contraction, involving the correlation between a charm and a light-quark loop. Cutoff effects turn out to be sizeable, which leads us to use lighter-than-physical charm masses, to employ a broad range of lattice spacings reaching down to 0.039 fm and to perform a combined charm-mass and continuum extrapolation. We use the [Formula: see text] meson to define the physical charm-mass point and obtain a final value of [Formula: see text] , whose uncertainty is dominated by the systematics of the extrapolation. Our result is consistent with the estimate based on a simple charm-quark loop, whilst being free of any perturbative scheme dependence on the charm mass. The mixed charm–light disconnected contraction contributes a small negative amount to the final value. |
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