Measurement of the $\nu_{\mu}$ charged-current cross sections on water, hydrocarbon, iron, and their ratios with the T2K on-axis detectors

K. Abe, R. Akutsu, A. Ali, C. Andreopoulos, L. Anthony, M. Antonova, S. Aoki, A. Ariga, Y. Ashida, Y. Awataguchi, Y. Azuma, S. Ban, M. Barbi, G. Barker, G. Barr, C. Barry, M. Batkiewicz-Kwasniak, F. Bench, V. Berardi, S. Berkman, R. Berner, L. Berns, S. Bhadra, S. Bienstock, A. Blondely, S. Bolognesi, B. Bourguille, S. Boyd, D. Brailsford, A. Bravar, C. Bronner, M. Avanzini, J. Calcutt, T. Campbell, S. Cao, S. Cartwright, M. Catanesi, A. Cervera, A. Chappell, C. Checchia, D. Cherdack, N. Chikuma, G. Christodoulouy, J. Coleman, G. Collazuol, D. Coplowe, A. Cudd, A. Dąbrowska, G. Rosa, T. Dealtry, P. Denner, S. Dennis, C. Densham, F. Lodovico, N. Dokania, S. Dolan, O. Drapier, K. Duffy, J. Dumarchez, P. Dunne, S. Emery-Schrenk, A. Ereditato, P. Fernández, T. Feusels, A. Finch, G. Fiorentini, G. Fiorillo, C. Francois, M. Friend, Y. Fujii, R. Fujita, D. Fukuda, Y. Fukuda, K. Gameil, C. Giganti, F. Gizzarelli, T. Golan, M. Gonin, D. Hadley, J. Haigh, P. Hamacher-Baumann, M. Hartz, T. Hasegawa, N. Hastings, T.
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引用次数: 3

Abstract

We report a measurement of the flux-integrated $\nu_{\mu}$ charged-current cross sections on water, hydrocarbon, and iron in the T2K on-axis neutrino beam with a mean neutrino energy of 1.5 GeV. The measured cross sections on water, hydrocarbon, and iron are $\sigma^{\rm{H_{2}O}}_{\rm{CC}}$ = (0.840$\pm 0.010$(stat.)$^{+0.10}_{-0.08}$(syst.))$\times$10$^{-38}$cm$^2$/nucleon, $\sigma^{\rm{CH}}_{\rm{CC}}$ = (0.817$\pm 0.007$(stat.)$^{+0.11}_{-0.08}$(syst.))$\times$10$^{-38}$cm$^2$/nucleon, and $\sigma^{\rm{Fe}}_{\rm{CC}}$ = (0.859$\pm 0.003$(stat.) $^{+0.12}_{-0.10}$(syst.))$\times$10$^{-38}$cm$^2$/nucleon respectively, for a restricted phase space of induced muons: $\theta_{\mu} $0.4 GeV/$c$ in the laboratory frame. The measured cross section ratios are ${\sigma^{\rm{H_{2}O}}_{\rm{CC}}}/{\sigma^{\rm{CH}}_{\rm{CC}}}$ = 1.028$\pm 0.016$(stat.)$\pm 0.053$(syst.), ${\sigma^{\rm{Fe}}_{\rm{CC}}}/{\sigma^{\rm{H_{2}O}}_{\rm{CC}}}$ = 1.023$\pm 0.012$(stat.)$\pm 0.058$(syst.), and ${\sigma^{\rm{Fe}}_{\rm{CC}}}/{\sigma^{\rm{CH}}_{\rm{CC}}}$ = 1.049$\pm 0.010$(stat.)$\pm 0.043$(syst.). These results, with an unprecedented precision for the measurements of neutrino cross sections on water in the studied energy region, show good agreement with the current neutrino interaction models used in the T2K oscillation analyses.
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测量$\nu_{\mu}$带电电流的横截面上的水,碳氢化合物,铁,和他们的比例与T2K轴探测器
我们报告了在平均中微子能量为1.5 GeV的T2K轴上中微子束中对水、碳氢化合物和铁的通量积分$\nu_{\mu}$带电电流截面的测量。测得的水、烃、铁的截面分别为$\sigma^{\rm{H_{2}O}}_{\rm{CC}}$ = (0.840 $\pm 0.010$ (stat.) $^{+0.10}_{-0.08}$ (syst.)) $\times$ 10 $^{-38}$ cm $^2$ /nucleon、$\sigma^{\rm{CH}}_{\rm{CC}}$ = (0.817 $\pm 0.007$ (stat.) $^{+0.11}_{-0.08}$ (syst.)) $\times$ 10 $^{-38}$ cm $^2$ /nucleon、$\sigma^{\rm{Fe}}_{\rm{CC}}$ = (0.859 $\pm 0.003$ (stat.) $^{+0.12}_{-0.10}$ (syst.)) $\times$ 10 $^{-38}$ cm $^2$ /nucleon。对于受限的诱导μ子相空间:$\theta_{\mu} $ 0.4 GeV/ $c$在实验室框架中。实测截面比分别为${\sigma^{\rm{H_{2}O}}_{\rm{CC}}}/{\sigma^{\rm{CH}}_{\rm{CC}}}$ = 1.028 $\pm 0.016$ (stat.) $\pm 0.053$ (syst.)、${\sigma^{\rm{Fe}}_{\rm{CC}}}/{\sigma^{\rm{H_{2}O}}_{\rm{CC}}}$ = 1.023 $\pm 0.012$ (stat.) $\pm 0.058$ (syst.)和${\sigma^{\rm{Fe}}_{\rm{CC}}}/{\sigma^{\rm{CH}}_{\rm{CC}}}$ = 1.049 $\pm 0.010$ (stat.) $\pm 0.043$ (syst.)。这些结果与目前用于T2K振荡分析的中微子相互作用模型具有良好的一致性,在所研究的能量区对水中中微子横截面的测量具有前所未有的精度。
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