Prospect of a very long baseline neutrino oscillation experiment
Lim Yuh Shan
Ching- Hsing Shen
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Semantic Scholar extracted view of "Prospect of a very long baseline neutrino oscillation experiment" by Hesheng Chen et al.
Baseline (configuration management)
Health Insurance Portability and Accountability Act
28 Figures and Tables
Figure 1: Summary of current experimental results on neutrino oscillations. Filled areas are allowed regions from the evidence of neutrino oscillations. Excluded regions are up and right of curves. Sensitivity curves of future experiments are also shown.
Table 1: Summary of neutrino oscillation experiments.
Table 2: Summary of mixing parameters of the three categories of neutrino oscillation experiments
Figure 2: Three possible level structures of the 3-neutrino scenario
Figure 3: Three possible level structures of the 4-neutrino scenario
Table 3: Numerical parameters for meson-neutrino energy spectrum
Table 4: Earth density versus the radius; x ≡ r/rE ,D ≡ rE − r.
Figure 4: Earth density profile.
Table 5: Summary of relative figure of merits for various measurement at baselines L=300 and 2100 km.
Figure 6: Figure of merit for sin2 2θ13 measurement at a) neutrino factories without backgrounds, b) meson-neutrino beams without backgrounds, c) neutrino factories with f=0.02 and r=0.1, and d) meson-neutrino beams with f=0.03 and r=0.1.
Table 6: Currently proposed detector for ν factories and conventional ν beams.
Figure 7: Figure of merit for CP phase measurement at a) neutrino factories with f=0.02 and r=0.1, and b) meson-neutrino beams with f=0.03 and r=0.1.
Table 7: Results from Monte Carlo simulation: Efficiency vs background rejection power for different flavors.
Figure 8: Figure of merit for the sign of ∆m232 at a) neutrino factories with f=0.02 and r=0.1, and b) meson-neutrino beams with f=0.03 and r=0.1.
Figure 9: Figure of merit for the matter effect at a) neutrino factories with f=0.02 and r=0.1, and b) meson-neutrino beams with f=0.03 and r=0.1.
Figure 10: Figure of merit for ∆m232 and sin 2 2θ23 at a) neutrino factories with f=0.01 and r=0.1, and b) meson-neutrino beams with f=0.01 and r=0.1.
Figure 11: Figure of merit for tau appearance at a) neutrino factories with f=0.03 and r=0.1, and b) meson-neutrino beams with f=0.03 and r=0.1.
Figure 12: Schematic of water Čerenkov calorimeter
Figure 13: Schematic of a water tank.
Figure 14: Schematic of a toroid magnet
Figure 15: A typical νµ CC events in the detector.
Figure 17: Beam profile of HIPA-Beijing
Figure 18: The maximum energy deposit in a cell normalized to the jet energy, Emax/Ejet, for various type of neutrino events.
Figure 19: The longitudinal length of a jet normalized to the jet energy, Lshower/Ejet, for various type of neutrino events.
Figure 20: The number of cells fired normalized to the jet energy, Ntank/Ejet, for various type of neutrino events
Figure 21: The transverse event size normalized to the total visible energy in the detector, Rxy/Etot, for various type of neutrino events.
Figure 22: The transverse event size at the shower maxima normalized to the total visible energy in the detector, Rmaxxy /Etot for various type of neutrino events. The distribution of νe is different from all the others.
Figure 23: Sensitivity to sin2 2θ13 at H2B.
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