Measurements of (nu)over-bar(mu) and (nu)over-bar(mu) + nu(mu) charged-current cross-sections without detected pions or protons on water and hydrocarbon at a mean anti-neutrino energy of 0.86 GeV

Abstract

International audienceWe report measurements of the flux-integrated |νμ\overline{\nu}_\mu| and |νμ+νμ\overline{\nu}_\mu+\nu_\mu| charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam with a mean beam energy of 0.86 GeV. The signal is defined as the (anti-)neutrino charged-current interaction with one induced |μ±\mu^\pm| and no detected charged pion or proton. These measurements are performed using a new WAGASCI module recently added to the T2K setup in combination with the INGRID Proton Module. The phase space of muons is restricted to the high-detection efficiency region, |pμ>400 MeV/cp_{\mu}>400~{\rm MeV}/c| and |θμ200 MeV/c\theta_{\mu}200~{\rm MeV}/c|⁠, |θπ600 MeV/c\theta_{\pi}600~{\rm MeV}/c|⁠, |θp<70\theta_{\rm p}<70^{\circ}| is required. In this paper, both the |νμ\overline{\nu}_\mu| cross-sections and |νμ+νμ\overline{\nu}_\mu+\nu_\mu| cross-sections on water and hydrocarbon targets and their ratios are provided by using the D’Agostini unfolding method. The results of the integrated |νμ\overline{\nu}_\mu| cross-section measurements over this phase space are |σH2O=(1.082±0.068(stat.)0.128+0.145(syst.))×1039cm2/nucleon\sigma_{\rm H_{2}O}=(1.082\pm0.068(\rm stat.)^{+0.145}_{-0.128}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}|⁠, |σCH=(1.096±0.054(stat.)0.117+0.132(syst.))×1039cm2/nucleon\sigma_{\rm CH}=(1.096\pm0.054(\rm stat.)^{+0.132}_{-0.117}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}|⁠, and |σH2O/σCH=0.987±0.078(stat.)0.090+0.093(syst.)\sigma_{\rm H_{2}O}/\sigma_{\rm CH} = 0.987\pm0.078(\rm stat.)^{+0.093}_{-0.090}(\rm syst.)|⁠. The |νμ+νμ\overline{\nu}_\mu+\nu_\mu| cross-section is |σH2O=(1.155±0.064(stat.)0.129+0.148(syst.))×1039cm2/nucleon\sigma_{\rm H_{2}O} = (1.155\pm0.064(\rm stat.)^{+0.148}_{-0.129}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}|⁠, |σCH=(1.159±0.049(stat.)0.115+0.129(syst.))×1039cm2/nucleon\sigma_{\rm CH}=(1.159\pm0.049(\rm stat.)^{+0.129}_{-0.115}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}|⁠, and |σH2O/σCH=0.996±0.069(stat.)0.078+0.083(syst.)\sigma_{\rm H_{2}O}/\sigma_{\rm CH}=0.996\pm0.069(\rm stat.)^{+0.083}_{-0.078}(\rm syst.)|⁠

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    Last time updated on 14/05/2020
    Last time updated on 14/05/2020