[1] Cleveland B T, Daily T, Davis R, et al.Measurement of the solar electron neutrino flux with the homestake chlorine detector [J].Astrophys J, 1988, 496: 505-526.
[2] Fukuda Y, Hayakawa T, Inoue K, et al., Solar neutrino data covering solar cycle 22 [J].Phys Rev Lett, 1996, 77: 1 683-1 686.
[3] Abdurashitov J N, Gavrin V N, Gorbachev V V, et al., Measurement of the solar neutrino capture rate with gallium metal.III.Results for the 2002-2007 data-taking period [J].Phys Rev C, 2009, 80: 015807.
[4] Anselmann P, Hampel W, Heusser G, et al., Solar neutrinos observed by GALLEX at Gran Sasso [J].Phys Lett B, 1992, 285: 376-389.
[5] Altmann M, Balata M, Belli P, et al., Complete results for five years of GNO solar neutrino observations [J].Phys Lett B, 2005, 616: 174-190.
[6] Fukuda S, Fukuda Y, Ishitsuka M, et al., Determination of solar neutrino oscillation parameters using 1496 days of Super-Kamiokande-I data [J].Phys Lett B, 2002, 539: 179-187.
[7] Ahmad Q R, Allen R C, Andersen T C, et al., Measurement of the Rate of ν_e+d→p+p+e^- interactions produced by B8 solar neutrinos at the Sudbury Neutrino Observatory [J].Phys Rev Lett, 2001, 87: 071301.
[8] Fukuda Y, Hayakawa T, Ichihara E, et al., Evidence for oscillation of atmospheric neutrinos [J].Phys Rev Lett, 1998, 81: 1 562-1 567.
[9] Eguchi K, Enomoto S, Furuno K, et al., First results from KamLAND: evidence for reactor antineutrino disappearance [J].Phys Rev Lett, 2003, 90: 021802.
[10] Abe Y, Aberle C, Akiri T, et al., Indication of reactorv_e disappearance in the Double Chooz Experiment [J].Phys Rev Lett, 2012, 108: 131801.
[11] An F P, Bai J Z, Balantekin A B, et al., Observation of electron-antineutrino disappearance at Daya Bay [J].Phys Rev Lett, 2012, 108: 171803.
[12] Ahn J K, Chebotaryov S, Choi J H, et al., Observation of reactor electron antineutrinos disappearance in the RENO experiment [J].Phys Rev Lett, 2012, 108: 191802.
[13] Ahn M H, Aliu E, Andringa S, et al., Measurement of neutrino oscillation by the K2K experiment [J].Phys Rev D, 2006, 74: 072003.
[14] Michael D G, Adamson P, Alexopoulos T, et al., Observation of muon neutrino disappearance with the MINOS detectors in the NuMI neutrino beam [J].Phys Rev Lett, 2006, 97: 191801.
[15] Abe K, Abgrall N, Ajima Y, et al., First muon-neutrino disappearance study with an off-axis beam [J].Phys Rev D, 2012, 85: 031103(R).
[16] Abe K, Hayato Y, Iida T, et al., Evidence for the appearance of atmospheric Tau neutrinos in super-kamiokande [J].Phys Rev Lett, 2013, 110: 181802.
[17] Harari H, Haut H, Weyers J.Quark masses and cabibbo angles [J].Phys Lett B, 1978, 78: 459-461.
[18] Froggatt C D, Nielsen H B.Hierarchy of quark masses, Cabibbo angles and CP violation [J].Nucl Phys B, 1979, 147: 277-298.
[19] Ishimori H, Kobayashi T, Ohki H, et al.Non-Abelian discrete symmetries in particle physics [J].Prog Theor Phys Suppl, 2010, 183: 1-163.
[20] Xing Z Z, Yang D, Zhou S.Broken S₃ flavor symmetry of leptons and quarks: mass spectra and flavor mixing patterns [J].Phys Lett B, 2010, 690: 304-310.
[21] Zhou S.Relatively large θ₁₃ and nearly maximal θ₂₃ from the approximate S₃ symmetry of lepton mass matrices [J].Phys Lett B, 2011, 704: 291-295.
[22] Fritzsch H, Xing Z Z.Lepton mass hierarchy and neutrino oscillations [J].Phys Lett B, 1996, 372: 265-270.
[23] Fritzsch H, Xing Z Z.Large leptonic flavor mixing and the mass spectrum of leptons [J].Phys Lett B, 1998, 440: 313-318.
[24] Fritzsch H, Xing Z Z.Maximal neutrino mixing and maximal CP violation [J].Phys Rev D, 2000, 61: 073016.
[25] Minkowski P. μ→eγ at a rate of one out of 10⁹ muon decays? [J].Phys Lett B, 1977, 67: 421-428.
[26] Mohapatra R N, Senjanovic G.Neutrino mass and spontaneous parity nonconservation [J].Phys Rev Lett, 1980, 44(14): 912-915.
[27] Konetschny W, Kummer W.Nonconservation of total lepton number with scalar bosons [J].Phys Lett B, 1977, 70: 433-435.
[28] Magg M, Wetterich C.Neutrino mass problem and gauge hierarchy [J].Phys Lett B, 1980, 94: 61-64.
[29] Schechter J, Valle J W F.Neutrino masses in SU(2)⊗U(1) theories [J].Phys Rev D, 1980, 22(9): 2 227-2 235.
[30] Cheng T P, Li L F.Neutrino masses, mixings, and oscillations in SU(2)×U(1) models of electroweak interactions [J].Phys Rev D, 1980, 22(11): 2 860-2 868.
[31] Lazarides G, Shafi Q, Wetterich C.Proton lifetime and fermion masses in an SO(10) model [J].Nucl Phys B, 1981, 181: 287-300.
[32] Mohapatra R N, Senjanovic G.Neutrino masses and mixings in gauge models with spontaneous parity violation [J].Phys Rev D, 1981, 23(1): 165-180.
[33] Foot R, Lew H, He X G, et al.See-saw neutrino masses induced by a triplet of leptons [J].Z Phys C, 1989, 44: 441-444.
[34] Fritzsch H, Xing Z Z.Democratic neutrino mixing reexamined [J].Phys Lett B, 2004, 598: 237-242.
[35] Maki Z, Nakagawa M, Sakata S.Remarks on the unified model of elementary particles [J].Prog Theor Phys, 1962, 28(5): 870-880.
[36] Olive K A, Agashe K, Amsler C, et al.Review of particle physics (particle data group)[J].Chin Phys C, 2014, 38(9): 090001.
[37] Jarlskog C.Commutator of the quark mass matrices in the standard electroweak model and a measure of maximal CP nonconservation [J].Phys Rev Lett, 1985, 55(10): 1 039-1 042.
[38] Wu D D.Rephasing invariants and CP violation [J].Phys Rev D, 1986, 33(3): 860-863.
[39] Gonzalez-Garcia M C, Maltoni M, Schwetz T.Updated fit to three neutrino mixing: status of leptonic CP violation [J].JHEP, 2014, 1411:052.
[40] Xing Z Z, Zhang H, Zhou S.Impacts of the Higgs mass on vacuum stability, running fermion masses, and two-body Higgs decays [J].Phys Rev D, 2012, 86: 013013.