Abstract

We report a measurement of the $\nu_{\mu}$-nucleus inclusive charged current cross section (=$\sigma^{cc}$) on iron using data from exposed to the J-PARC neutrino beam. The detector consists of 14 modules in total, which are spread over a range of off-axis angles from 0$^\circ$ to 1.1$^\circ$. The variation in the neutrino energy spectrum as a function of the off-axis angle, combined with event topology information, is used to calculate this cross section as a function of neutrino energy. The cross section is measured to be $\sigma^{cc}(1.1\text{ GeV}) = 1.10 \pm 0.15$ $(10^{-38}\text{cm}^2/\text{nucleon})$, $\sigma^{cc}(2.0\text{ GeV}) = 2.07 \pm 0.27$ $(10^{-38}\text{cm}^2/\text{nucleon})$, and $\sigma^{cc}(3.3\text{ GeV}) = 2.29 \pm 0.45$ $(10^{-38}\text{cm}^2/\text{nucleon})$, at energies of 1.1, 2.0, and 3.3 GeV, respectively. These results are consistent with the cross section calculated by the neutrino interaction generators currently used by T2K. More importantly, the method described here opens up a new way to determine the energy dependence of neutrino-nucleus cross sections.

Highlights

  • Many recent long baseline neutrino oscillation experiments use muon-neutrino beams, with neutrino energies ranging from sub-GeV to a few GeV

  • We report a measurement of the νμ-nucleus inclusive charged-current cross section (1⁄4 σcc) on iron using data from the INGRID detector exposed to the J-PARC neutrino beam

  • Neutrino-nucleus (Fe) interactions in the INGRID module are simulated by a neutrino event generator, which is a composite of different neutrino interaction models

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Summary

INTRODUCTION

Many recent long baseline neutrino oscillation experiments use muon-neutrino beams, with neutrino energies ranging from sub-GeV to a few GeV. Neutrino beams which cover the few-GeV region The former experiment measured the CC inclusive cross section for neutrinos with energies above 3.5 GeV using the MINOS near detector. We present a measurement of the νμ inclusive CC cross section on iron in the energy range of 1–3 GeV with INGRID. This analysis uses data collected from 2010 to 2013, corresponding to 6.27 × 1020 protons on target (POT). The neutrino interactions at different INGRID modules, which are distributed at different positions and observed different beam spectra, is used to extract the energy dependence of the cross section.

THE T2K NEAR DETECTOR
SIMULATING NEUTRINO INTERACTIONS IN THE INGRID DETECTOR
Flux prediction
Flux uncertainties
The NEUT neutrino event generator
Neutrino-nucleus interaction simulation
Neutrino interaction model uncertainties
Detector simulation
Overview
Neutrino event selection
Event topology
Module grouping
Detector response uncertainties
Cross-section extraction
Correlated errors χ2
Δfbig i
Energy binning
PROPAGATION OF SYSTEMATIC UNCERTAINTIES
Systematics uncertainty on NC interactions
Systematic uncertainty on CC interactions
Systematic uncertainty on FSI
Uncertainty in pion multiplicities and secondary interactions
RESULT
Cross-section fit
Summary
Findings
CONCLUSION
Full Text
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