T2K · 2021

Measurements of νμ\overline{\nu}_{\mu} and νμ+νμ\overline{\nu}_{\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

PTEP 2021 043C01 · 10.1093/ptep/ptab014

Measurements

CurrentFlavorTargetTopologyTypeObservablesEnergy
CCνμ, ν̄μH2O, CHCC0πratiocross sections and ratiomean energy 0.86GeV

Abstract

We report measurements of the flux-integrated νˉμ\bar{\nu}_\mu and νˉμ+νμ\bar{\nu}_\mu+\nu_\mu charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam, with a mean neutrino 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 nor 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 θμ<30\theta_{\mu}<30^{\circ}, in the laboratory frame. Absence of pions and protons in the detectable phase space of "pπ>200 MeV/cp_{\pi}>200~{\rm MeV}/c and θπ<70\theta_{\pi}<70^{\circ}", and "pp>600 MeV/cp_{\rm p}>600~{\rm MeV}/c and θp<70\theta_{\rm p}<70^{\circ}" is required. In this paper, both of the νˉμ\bar{\nu}_\mu cross-sections and νˉμ+νμ\bar{\nu}_\mu+\nu_\mu cross-sections on water and hydrocarbon targets, and their ratios are provided by using D'Agostini unfolding method. The results of the integrated νˉμ\bar{\nu}_\mu cross-section measurements over this phase space are σH2O=(1.082±0.068(stat.)0.128+0.145(syst.))×1039 cm2/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.))×1039 cm2/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 νˉμ+νμ\bar{\nu}_\mu+\nu_\mu cross-section is σH2O=(1.155±0.064(stat.)0.129+0.148(syst.))×1039 cm2/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.))×1039 cm2/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.).

Citation

@article{T2K:2020txr,
    author = "Abe, K. and others",
    collaboration = "T2K",
    title = "{Measurements of $\overline{\nu}_{\mu}$ and $\overline{\nu}_{\mu} + \nu_{\mu}$ charged-current cross-sections without detected pions or protons on water and hydrocarbon at a mean anti-neutrino energy of 0.86 GeV}",
    eprint = "2004.13989",
    archivePrefix = "arXiv",
    primaryClass = "hep-ex",
    doi = "10.1093/ptep/ptab014",
    journal = "PTEP",
    volume = "2021",
    number = "4",
    pages = "043C01",
    year = "2021"
}