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Charged lepton contributions to the solar neutrino mixing and
Phys. Rev. D 70, 013003 – Published 27 July, 2004
DOI: https://doi.org/10.1103/PhysRevD.70.013003
Abstract
A charged lepton contribution to the solar neutrino mixing induces a contribution to barring cancellations or correlations, which is independent of the model building options in the neutrino sector. We illustrate two robust arguments for that contribution to be within the expected sensitivity of high intensity neutrino beam experiments. We find that the case in which the neutrino sector gives rise to a maximal solar angle (the natural situation if the hierarchy is inverse) leads to a close to or exceeding the experimental bound depending on the precise values of an unknown phase and possible additional contributions. We finally discuss the possibility that the solar angle originates predominantly in the charged lepton sector. We find that the construction of a model of this sort is more complicated. We comment on a recent example of natural model of this type.
References (19)
- R. Barbieri, T. Hambye, and A. Romanino, J. High Energy Phys. 03, 017 (2003).
- E.K. Akhmedov, G.C. Branco, and M.N. Rebelo, Phys. Rev. Lett. 84, 3535 (2000).
- S.M. Barr and I. Dorsner, Nucl. Phys. B585, 79 (2000).
- F. Feruglio, A. Strumia, and F. Vissani, Nucl. Phys. B637, 345 (2002).
- S. Lavignac, I. Masina, and C.A. Savoy, Nucl. Phys. B633, 139 (2002).
- P.H. Frampton, S.T. Petcov, and W. Rodejohann, Nucl. Phys. B687, 31 (2004).
- R. Kuchimanchi and R.N. Mohapatra, Phys. Lett. B 552, 198 (2003).
- R. Barbieri, P. Creminelli, and A. Romanino, Nucl. Phys. B559, 17 (1999).
- A. Ibarra and G.G. Ross, Phys. Lett. B 575, 279 (2003).
- R.F. Lebed and D.R. Martin, hep-ph/0312219.
- S.F. King and N.N. Singh, Nucl. Phys. B596, 81 (2001).
- S.F. King, J. High Energy Phys. 09, 011 (2002).
- The present paper is based on a talk first given at CERN in September 2003.
- G. Altarelli, F. Feruglio, and I. Masina, Nucl. Phys. B689, 157 (2004).
- A.Y. Smirnov, Phys. Rev. D 48, 3264 (1993); S.F. King, Phys. Lett. B 439, 350 (1998); ibid.S. Davidson and S.F. King, 445, 191 (1998); ibid.R. Barbieri, L.J. Hall, and A. Strumia, 445, 407 (1999); ibid.Q. Shafi and Z. Tavartkiladze, 451, 129 (1999); S.F. King, Nucl. Phys. B562, 57 (1999); G. Altarelli, F. Feruglio, and I. Masina, Phys. Lett. B 472, 382 (2000); S.F. King, Nucl. Phys. B576, 85 (2000).
- C.H. Albright and S.M. Barr, Phys. Rev. D 58, 013002 (1998); C.H. Albright, K.S. Babu, and S.M. Barr, Phys. Rev. Lett. 81, 1167 (1998); G. Altarelli and F. Feruglio, Phys. Lett. B 439, 112 (1998); ibid.P.H. Frampton and A. Rasin, 478,424 (2000).
- S.F. King, Rep. Prog. Phys. 67, 107 (2004).
- R. Gatto, G. Sartori, and M. Tonin, Phys. Lett. 28B, 128 (1968); ibid.R.J. Oakes, 29B, 683 (1969); ibid.30B, 262 (1969).
- R. Barbieri, L.J. Hall, S. Raby, and A. Romanino, Nucl. Phys. B493, 3 (1997).