17 research outputs found
Uncertainties on the /, / and / cross-section ratio from the modelling of nuclear effects and their impact on neutrino oscillation experiments
Recent studies have demonstrated non-trivial behaviours in the cross-section
extrapolation from () to
() interactions on nuclear targets in the charged-current
quasi-elastic (CCQE) regime. In this article, the potential for mis-modeling of
/, / and
/ cross-section ratios due to nuclear effects is
quantified by considering the model spread within the full kinematic phase
space for CCQE interactions. Its impact is then propagated to a simulated
experimental configuration based on the Hyper-K experiment, which is dominated
by CCQE interactions. Although a relatively large discrepancy between
theoretical models is confirmed for forward lepton angles at neutrino energies
below 300 MeV and for a new region of phase space at lepton angles above
, both regions are demonstrated to contribute a very small portion
of the Hyper-K (or T2K) flux integrated cross section. Overall, a systematic
uncertainty on the oscillated flux-averaged /
cross-section ratio is estimated to be 2%. A similar study was also
conducted for the proposed lower-energy ESSSB experiment configuration,
where the resulting uncertainty was found to be larger.Comment: 14 pages, 10 figures. Fixed abstract misformating on arxiv pag
Uncertainties on the ν (-) e/ ν (-) μ and νe/ ν ¯ e cross-section ratio from the modeling of nuclear effects at 0.2 to 1.2 GeV neutrino energies and their impact on neutrino oscillation experiments
The potential for mismodeling of νμ/νe, ν¯μ/ν¯e, and νe/ν¯e cross-section ratios due to nuclear effects is quantified by considering model spread within the full kinematic phase space for charged-current quasielastic interactions. Its impact is then propagated to simulated experimental configurations based on the Hyper-K and ESSνSB experiments. Although significant discrepancies between theoretical models is confirmed, it is found that these largely lie in regions of phase space that contribute only a very small portion of the flux-integrated cross sections. Overall, a systematic uncertainty on the oscillated flux-averaged νe/ν¯e cross-section ratio is found to be ∼2 and ∼4% for Hyper-K and ESSνSB, respectively.ISSN:1550-7998ISSN:0556-2821ISSN:1550-236
Uncertainties on the and cross-section ratio from the modeling of nuclear effects at 0.2 to 1.2 GeV neutrino energies and their impact on neutrino oscillation experiments
The potential for mismodeling of νμ/νe, ¯νμ/¯νe, and νe/¯νe cross-section ratios due to nuclear effects is quantified by considering model spread within the full kinematic phase space for charged-current quasielastic interactions. Its impact is then propagated to simulated experimental configurations based on the Hyper-K and ESSνSB experiments. Although significant discrepancies between theoretical models is confirmed, it is found that these largely lie in regions of phase space that contribute only a very small portion of the flux-integrated cross sections. Overall, a systematic uncertainty on the oscillated flux-averaged νe/¯νe cross-section ratio is found to be ∼2 and ∼4% for Hyper-K and ESSνSB, respectively
Uncertainties on the /, / and / cross-section ratio from the modelling of nuclear effects and their impact on neutrino oscillation experiments
International audienceRecent studies have demonstrated non-trivial behaviours in the cross-section extrapolation from () to () interactions on nuclear targets in the charged-current quasi-elastic (CCQE) regime. In this article, the potential for mis-modeling of /, / and / cross-section ratios due to nuclear effects is quantified by considering the model spread within the full kinematic phase space for CCQE interactions. Its impact is then propagated to a simulated experimental configuration based on the Hyper-K experiment, which is dominated by CCQE interactions. Although a relatively large discrepancy between theoretical models is confirmed for forward lepton angles at neutrino energies below 300 MeV and for a new region of phase space at lepton angles above , both regions are demonstrated to contribute a very small portion of the Hyper-K (or T2K) flux integrated cross section. Overall, a systematic uncertainty on the oscillated flux-averaged / cross-section ratio is estimated to be 2%. A similar study was also conducted for the proposed lower-energy ESSSB experiment configuration, where the resulting uncertainty was found to be larger