2009
DOI: 10.1103/physrevd.79.072002
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Neutrino flux prediction at MiniBooNE

Abstract: The Booster Neutrino Experiment (MiniBooNE) searches for ν µ → ν e oscillations using the O(1 GeV) neutrino beam produced by the Booster synchrotron at the Fermi National Accelerator Laboratory (FNAL). The Booster delivers protons with 8 GeV kinetic energy (8.89 GeV/c momentum) to a beryllium target, producing neutrinos from the decay of secondary particles in the beam line. We describe the Monte Carlo simulation methods used to estimate the flux of neutrinos from the beamline incident on the MiniBooNE detecto… Show more

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Cited by 440 publications
(729 citation statements)
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“…The most important external source of neutrino data for our interaction model parameter constraints is the MiniBooNE experiment [37]. The MiniBooNE flux [38] covers an energy range similar to that of T2K and, as a 4π detector like SK, has a similar phase space acceptance, meaning NEUT is tested over a broader range of Q 2 than current ND280 analyses.…”
Section: B Constraints From External Experimentsmentioning
confidence: 99%
“…The most important external source of neutrino data for our interaction model parameter constraints is the MiniBooNE experiment [37]. The MiniBooNE flux [38] covers an energy range similar to that of T2K and, as a 4π detector like SK, has a similar phase space acceptance, meaning NEUT is tested over a broader range of Q 2 than current ND280 analyses.…”
Section: B Constraints From External Experimentsmentioning
confidence: 99%
“…The MicroBooNE detector [5] consists of a rectangular time-projection chamber (TPC) with dimensions 2.6 m × 2.3 m × 10.4 m (width × height × length) located 470 m downstream from the Booster Neutrino Beam (BNB) target [6]. LArTPCs allow for precise three-dimensional reconstruction of particle interactions.…”
Section: Introductionmentioning
confidence: 99%
“…Typically, experiments rely on measurements of the pion and kaon spectra made by dedicated particle production experiments to predict their neutrino flux, resulting in significant uncertainties in the flux and hence in the measured cross sections. [19,20] Thus, it is ideal to measure the neutrino flux from the beamline data itself.…”
Section: Goal Of This Thesismentioning
confidence: 99%