E-viri
  • Measurement of parameters
    Anashin, V V; Aulchenko, V M; Baldin, E M; Barladyan, A K; Barnyakov, AYu; Barnyakov, MYu; Baru, SE; Basok, IYu; Beloborodova, O L; Blinov, A E; Blinov, V E; Bobrov, A V; Bobrovnikov, V S; Bogomyagkov, A V; Bondar, A E; Buzykaev, A R; Eidelman, SI; Grigoriev, D N; Glukhovchenko, YuM; Gulevich, V V; Gusev, D V; Karnaev, SE; Karpov, G V; Karpov, S V; Kharlamova, T A; Kiselev, V A; Kolmogorov, V V; Kononov, SA; Kotov, KYu; Kravchenko, E A; Kulikov, V F; Kurkin, GYa; Kuper, E A; Levichev, E B; Maksimov, DA; Malyshev, V M; Maslennikov, AL; Medvedko, A S; Meshkov, OI; Mishnev, SI; Morozov, I I; Muchnoi, NYu; Neufeld, V V; Nikitin, SA; Nikolaev, IB; Okunev, IN; Onuchin, A P; Oreshkin, S B; Orlov, I O; Osipov, A A

    Physics letters. B, 05/2012, Letnik: 711, Številka: 3-4
    Journal Article

    We report the final results of a study of the psi ( 3770 ) meson using a data sample collected with the KEDR detector at the VEPP-4M electron-positron collider. The data analysis takes into account interference between the resonant and nonresonant D D macr production, where the latter is related to the nonresonant part of the energy-dependent form factor F D . The vector dominance approach and several empirical parameterizations have been tried for the nonresonant F D N R ( s ) . Our results for the mass and total width of psi ( 3770 ) are M = 3779.2 - 1.7 + 1.8 - 0.7 + 0.5 - 0.3 + 0.3 MeV , Gamma = 24.9 - 4.0 + 4.6 - 0.6 + 0.5 - 0.9 + 0.2 MeV , where the first, second and third uncertainties are statistical, systematic and model, respectively. For the electron partial width two possible solutions have been found: ( 1 ) Gamma e e = 154 - 58 + 79 - 9 + 17 - 25 + 13 eV , ( 2 ) Gamma e e = 414 - 80 + 72 - 26 + 24 - 10 + 90 eV . Our statistics are insufficient to prefer one solution to another. The Solution (2) mitigates the problem of non- D D macr decays but is disfavored by potential models. It is shown that taking into account the resonance-continuum interference in the near-threshold region affects resonance parameters, thus the results presented cannot be directly compared with the corresponding PDG values obtained ignoring this effect.