1999
DOI: 10.1142/s0217751x99000981
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Analysis of Neutrino Oscillation in Three-Flavor Neutrinos

Abstract: We analyzed the solar, terrestrial and atmospheric neutrinos experiments using the three-flavor neutrino framework and got the allowed regions for param- is favored than the small angle slution from the analysis of zenith angle dependence in atmospheric neutrino sub-GeV experiment.

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Cited by 16 publications
(3 citation statements)
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“…set by the CHOOZ [19] long baseline reactor in the disappearance mode ν e → ν x , an analysis in Ref. [6] also has given allowed ranges of δ 2 and sin 2 2θ for φ < 20 • . Note that to zeroth order of δ 2 /∆ 2 , the probability becomes [18] P (ν e → ν e ) ≃ cos 4 φP 2ν + sin 4 φ.…”
Section: A Sn Neutrinos and Neutrino Parametersmentioning
confidence: 99%
See 1 more Smart Citation
“…set by the CHOOZ [19] long baseline reactor in the disappearance mode ν e → ν x , an analysis in Ref. [6] also has given allowed ranges of δ 2 and sin 2 2θ for φ < 20 • . Note that to zeroth order of δ 2 /∆ 2 , the probability becomes [18] P (ν e → ν e ) ≃ cos 4 φP 2ν + sin 4 φ.…”
Section: A Sn Neutrinos and Neutrino Parametersmentioning
confidence: 99%
“…The flavor oscillation can be parameterized by the mass-squared differences of the neutrino mass eigenstates ∆m 2 ≡ m 2 i − m 2 j (i, j = 1, 2, 3) and θ ij , the mixing angles between weak eigenstates and mass eigenstates of the neutrinos (θ ij ≤ π 4 is assumed). In terms of these parameters, the just-so vacuum oscillation [4] requires 6 × 10 −11 ≤ ∆m 2 ≤ 60 × 10 −11 eV 2 and sin 2 2θ ≃ 1, while the MSW resonant effect [5] in the Sun becomes important if 4 × 10 −6 eV 2 ≤ ∆m 2 ≤ 7 × 10 −5 eV 2 , sin 2 2θ ≃ 0.6 − 0.9 (large angle solution), or 3 × 10 −6 eV 2 ≤ ∆m 2 ≤ 12 × 10 −6 eV 2 , 0.003 ≤ sin 2 2θ ≤ 0.01 (small angle solution) [6]. Recent atmospheric neutrino data from the Super-Kamiokande [7] further provide a strong evidence in support of neutrino oscillation as the cause to deficit of muon neutrinos, provided ∆m 2 ∼ 10 −2 − 10 −3 eV 2 and sin 2 2θ > 0.82.…”
Section: Introductionmentioning
confidence: 99%
“…There have been many analytic works on three-flavor MSW solutions of the solar neutrino problem with simple linear and exponential matter densities [33][34][35][36][37][38][39][40]. Most three-flavor MSW fits to the solar neutrino experiments have been made within the above framework [41][42][43][44][45]. Recently exact solutions to the three neutrino MSW equations for such simple matter densities were derived [46][47][48].…”
Section: Introductionmentioning
confidence: 99%