Reactor measurement of θ_{12}; Secret of the power
arXiv:hep-ph/0501250 · doi:10.1016/j.nuclphysbps.2005.03.032
Abstract
We demonstrate enormous power of dedicated reactor experiment for θ_{12} with a detector placed at around the first oscillation maximum, which we call "SADO". It allows determination of sin^2θ_{12} to the accuracy of \simeq 2% at 1 σCL, which surpasses all the method so far proposed. Unlike reactor θ_{13} experiments, the requirement for the systematic error is very mild, \simeq 4%, which makes it an even more feasible experiment. If we place a detector at \sim 60 km away from the Kashiwazaki-Kariwa nuclear power plant, 0.5 kt yr exposure of SADO is equivalent to \sim 100 kt yr exposure of KamLAND assuming the same systematic error.
Addendum to hep-ph/0407326 with 3 new figures, based on talk at NOW2004
References in corpus (5)
- Big Bang Nucleosynthesis (in "The Review of Particle Properties" 2004)
- Measurement of Neutrino Oscillation with KamLAND: Evidence of Spectral Distortion
- High Precision Measurements of in Solar and Reactor Neutrino Experiments
- Reactor Measurement of theta_12; Principles, Accuracies and Physics Potentials
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Cited by in corpus (8)
- Resolving theta_{23} Degeneracy by Accelerator and Reactor Neutrino Oscillation Experiments
- Determination of the Neutrino Mass Hierarchy via the Phase of the Disappearance Oscillation Probability with a Monochromatic \barν_e Source
- Determining Neutrino Mass Hierarchy by Precision Measurements in Electron and Muon Neutrino Disappearance Experiments
- Recoilless Resonant Absorption of Monochromatic Neutrino Beam for Measuring Delta m^2_{31} and theta_{13}
- Testing CPT Symmetry with Supernova Neutrinos
- Random magnetic fields inducing solar neutrino spin-flavor precession in a three generation context
- Reactor Neutrino Experiments with a Large Liquid Scintillator Detector
- Probing Extra Dimensions with Neutrino Oscillations