Abstract

The Charged-Current Quasi-Elastic (CCQE) interaction, $\nu_{l} + n \rightarrow l^{-} + p$, is the dominant CC process at $E_\nu \sim 1$ GeV and contributes to the signal in accelerator-based long-baseline neutrino oscillation experiments operating at intermediate neutrino energies. This paper reports a measurement by the T2K experiment of the $\nu_{\mu}$ CCQE cross section on a carbon target with the off-axis detector based on the observed distribution of muon momentum ($p_\mu$) and angle with respect to the incident neutrino beam ($\theta_\mu$). The flux-integrated CCQE cross section was measured to be $(0.83 \pm 0.12) \times 10^{-38}\textrm{ cm}^{2}$ in good agreement with NEUT MC value of ${0.88 \times 10^{-38}} \textrm{ cm}^{2}$. The energy dependence of the CCQE cross section is also reported. The axial mass, $M_A^{QE}$, of the dipole axial form factor was extracted assuming the Smith-Moniz CCQE model with a relativistic Fermi gas nuclear model. Using the absolute (shape-only) $p_{\mu}cos\theta_\mu$ distribution, the effective $M_A^{QE}$ parameter was measured to be ${1.26^{+0.21}_{-0.18} \textrm{ GeV}/c^{2}}$ (${1.43^{+0.28}_{-0.22} \textrm{ GeV}/c^{2}}$).

Highlights

  • The charged-current quasielastic (CCQE) interaction, νl þ n → l− þ p, is the dominant CC process for neutrino-nucleon interactions at Eν ∼ 1 GeV and contributes to the total cross section in the neutrino energy range relevant for current accelerator-based long-baseline neutrino oscillation experiments

  • This paper reports a measurement by the T2K experiment of the νμ charged current quasielastic (CCQE) cross section on a carbon target with the off-axis detector based on the observed distribution of muon momentum and angle with respect to the incident neutrino beam

  • The CCQE interaction of a neutrino with a nucleon is a two-body interaction, and the initial neutrino energy can be estimated from relatively well-measured final state lepton kinematics without relying on reconstruction and energy measurement of the hadronic final state

Read more

Summary

INTRODUCTION

The charged-current quasielastic (CCQE) interaction, νl þ n → l− þ p, is the dominant CC process for neutrino-nucleon interactions at Eν ∼ 1 GeV and contributes to the total cross section in the neutrino energy range relevant for current accelerator-based long-baseline neutrino oscillation experiments. The MINOS experiment reports 1.23 Æ 0.20 GeV=c2 with an iron target with hEνi ∼ 2.8 GeV [9] These discrepancies have motivated theoretical work on more sophisticated models including contributions from multinucleon interactions which mimic the CCQE signal if the additional nucleons are not detected. Such additional processes contribute to the measured total cross section and can affect the neutrino energy reconstruction These new models have had success in describing MiniBooNE CCQE data [13,14,15,16,17] and T2K CC data [18,19,20,21,22].

THE T2K BEAM
THE OFF-AXIS ND280 DETECTOR
C H O Ti Si N
EVENT SELECTION
NEUTRINO INTERACTION MODEL
SYSTEMATIC UNCERTAINTIES
Neutrino beam flux uncertainty
Interaction model uncertainty
Detector response uncertainty
Methodology
Etνruebins eveX nt type
Background
Flux averaged total cross section
MQA E extraction
Findings
VIII. SUMMARY
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.