Contribution of Neutral Pseudoscalar Mesons to $ a \Mu^{Hlbl} $ Within
HLbL Contribution of neutral pseudoscalar mesons to aµ within a Schwinger-Dyson equations approach to QCD Kh´epaniRaya,1, ∗ Adnan Bashir,2, y and Pablo Roig3, z 1School of Physics, Nankai University, Tianjin 300071, China 2Instituto de F´ısica y Matem´aticas, Universidad Michoacana de San Nicol´asde Hidalgo, Morelia, Michoac´an58040, M´exico. 3Centro de Investigaci´ony de Estudios Avanzados, Apartado Postal 14-740, 07000, Ciudad de M´exico, M´exico (Dated: April 2, 2020) A continuum approach to Quantum Chromodynamics (QCD), based upon Schwinger-Dyson (SD) and Bethe-Salpeter (BS) equations, is employed to provide a tightly constrained prediction for the ∗ ∗ 0 0 γ γ ! fπ ; η; η ; ηc; ηbg transition form factors (TFFs) and their corresponding pole contribution to the hadronic light-by-light (HLbL) piece of the anomalous magnetic moment of the muon (aµ). This work relies on a practical and well-tested quark-photon vertex Ansatz approach to evaluate the TFFs for arbitrary space-like photon virtualities, in the impulse approximation. The numerical results are parametrized meticulously, ensuring a reliable evaluation of the HLbL contributions π0−pole −10 η−pole −10 η0−pole to aµ. We obtain: aµ = (6:14 ± 0:21) × 10 , aµ = (1:47 ± 0:19) × 10 , aµ = −10 π0+η+η0−pole −10 (1:36±0:08)×10 , yielding a total value of aµ = (8:97±0:48)×10 , compatible with ηc+ηb−pole ηc−pole −10 contemporary determinations. Notably, we find that aµ ≈ aµ = (0:09 ± 0:01) × 10 , which might not be negligible once the percent precision in the computation of the light pseudoscalars is reached.
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