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  • Aggarwal, L; Aloisio, A; Asner, D M; Aushev, V; Bahinipati, S; Baur, A; Beaubien, A; Bertacchi, V; Bessner, M; Bilka, T; Bobrov, A; Bozek, A; Browder, T E; Campajola, M; Cheema, P; Chilikin, K; H -E Cho; Cho, K; S -J Cho; S -K Choi; Dattola, F; De Pietro, G; Dhamija, R; F Di Capua; Dorigo, M; Dreyer, S; Dujany, G; ti, F; Fulsom, B G; Gabrielli, A; Gaudino, G; Gaz, A; Ghumaryan, H; Giri, A; Godang, R; Gogota, O; Granderath, S; Iijima, T; Ipsita, N; Jin, Y; Kaliyar, A B; Kandra, J; Kawasaki, T; Keil, F; Kim, D Y; K -H Kim; Križan, P; Kumara, K; Lacaprara, S; Le Diberder, F R; Y Li; Liu, Z Q; Liventsev, D; Lueck, T; Maity, S; Manfredi, R; Marcantonio, D; Massaccesi, L; Masuda, M; Mehta, R; Mitra, S; Miyabayashi, K; Mohanty, G B; Nazaryan, G; Ogawa, S; Patra, S; Pedlar, T K; Peschke, R; Pestotnik, R; G Pinna Angioni; Prim, M T; Rados, P; Raeuber, G; Raiz, S; Rauls, N; Rizzo, G; Sanders, D A; Sandilya, S; Schwanda, C; Sfienti, C; Shwartz, B; Skorupa, J; Spataro, S; Starič, M; Sumisawa, K; Suwonjandee, N; Tamponi, U; Tanida, K; Tonelli, D; Torassa, E; Trabelsi, K; Uematsu, Y; Varvell, K E; Vitale, L; Wang, E; M -Z Wang; Wessel, C; Yang, S B; Zhilich, V; Zhukova, V I

    arXiv.org, 04/2024
    Paper

    We report a measurement of the \(e^+e^- \to \pi^+\pi^-\pi^0\) cross section in the energy range from 0.62 to 3.50 GeV using an initial-state radiation technique. We use an \(e^+e^-\) data sample corresponding to 191 \(\text{fb}^{-1}\) of integrated luminosity, collected at a center-of-mass energy at or near the \(\Upsilon{(4S)}\) resonance with the Belle II detector at the SuperKEKB collider. Signal yields are extracted by fitting the two-photon mass distribution in \(e^+e^- \to \pi^+\pi^-\pi^0\gamma\) events, which involve a \(\pi^0 \to \gamma\gamma\) decay and an energetic photon radiated from the initial state. Signal efficiency corrections with an accuracy of 1.6% are obtained from several control data samples. The uncertainty on the cross section at the \(\omega\) and \(\phi\) resonances is dominated by the systematic uncertainty of 2.2%. The resulting cross sections in the 0.62-1.80 GeV energy range yield \( a_\mu^{3\pi} = 48.91 \pm 0.23~(\mathrm{stat}) \pm 1.07~(\mathrm{syst}) \times 10^{-10} \) for the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment. This result differs by \(2.5\) standard deviations from the most precise current determination.