Issue |
EPJ Web Conf.
Volume 179, 2018
International Workshop on “Flavour Changing and Conserving Processes” (FCCP2017)
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Article Number | 01016 | |
Number of page(s) | 6 | |
DOI | https://doi.org/10.1051/epjconf/201817901016 | |
Published online | 23 May 2018 |
https://doi.org/10.1051/epjconf/201817901016
Hadronic Leading Order Contribution to the Muon g-2
1
KEK Theory Center, Tsukuba, Ibaraki, 305-0801 Japan
2
Yukawa Institute for Theoretical Physics, Kyoto University, Kyoto, 606-8502, Japan
* e-mail: dnomura@post.kek.jp
Published online: 23 May 2018
We calculate the Standard Model (SM) prediction for the muon anomalous magnetic moment. By using the latest experimental data for e+e- → hadrons as input to dispersive integrals, we obtain the values of the leading order (LO) and the next-to-leading-order (NLO) hadronic vacuum polarisation contributions as ahad, LO VPμ = (693:27 ± 2:46) × 10-10 and ahad, NLO VP μ = (_9.82 ± 0:04) × 1010-10, respectively. When combined with other contributions to the SM prediction, we obtain aμ(SM) = (11659182:05 ± 3.56) × 10-10; which is deviated from the experimental value by Δaμ(exp) _ aμ(SM) = (27.05 ± 7.26) × 10-10. This means that there is a 3.7 σ discrepancy between the experimental value and the SM prediction. We also discuss another closely related quantity, the running QED coupling at the Z-pole, α(M2 Z). By using the same e+e- → hadrons data as input, our result for the 5-flavour quark contribution to the running QED coupling at the Z pole is Δ(5)had(M2 Z) = (276.11 ± 1.11) × 10-4, from which we obtain Δ(M2 Z) = 128.946 ± 0.015.
© The Authors, published by EDP Sciences, 2018
This is an Open Access article distributed under the terms of the Creative Commons Attribution License 4.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. (http://creativecommons.org/licenses/by/4.0/).
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