On the atmospheric neutrino oscillations, theta(13) and neutrino mass hierarchy
dc.contributor.area | Physics | en_US |
dc.contributor.author | Petcov, Serguey T. | en_US |
dc.contributor.author | Palomares-Ruiz, Sergio | en_US |
dc.contributor.department | Elementary Particle Theory | en_US |
dc.date.accessioned | 2007-11-14T10:32:54Z | en_US |
dc.date.accessioned | 2011-09-07T20:26:39Z | |
dc.date.available | 2007-11-14T10:32:54Z | en_US |
dc.date.available | 2011-09-07T20:26:39Z | |
dc.date.issued | 2007-11-14T10:32:54Z | en_US |
dc.description.abstract | We give predictions for the up-down asymmetry in the Nadir angle dependence of the ratio Nmu/Ne of the rates of the mu-like and e-like multi-GeV events measured in water-Cerenkov detectors (Super-Kamiokande, etc.) in the case of 3-neutrino oscillations of the atmospheric nu_e (antinu_e) and nu_mu (antinu_mu), driven by one neutrino mass squared difference, |Delta m^2_{atm}| = |Delta m^2_{31}| ~ (2.0 - 3.0) 10^{-3} eV^2 >> Delta m^2_{21} = Delta m^2_{sol}. This ratio is particularly sensitive to the Earth matter effects in the atmospheric neutrino oscillations, and thus to the values of sin^2(theta13) and sin^2(theta23), theta13 and theta23 being the neutrino mixing angle limited by the CHOOZ and Palo Verde experiments and that responsible for the dominant atmospheric nu_mu -> nu_tau (antinu_mu -> antinu_tau) oscillations, respectively. It is also sensitive to the type of neutrino mass spectrum which can be with normal (Delta m^2_{atm} > 0) or with inverted (Delta m^2_{atm} < 0) hierarchy. | en_US |
dc.format.extent | 122809 bytes | en_US |
dc.format.mimetype | application/pdf | en_US |
dc.identifier.uri | https://openscience.sissa.it/handle/1963/2416 | en_US |
dc.language.iso | en_US | en_US |
dc.relation.ispartofseries | SISSA;38/2004/EP | en_US |
dc.relation.ispartofseries | arXiv.org;hep-ph/0406106v1 | en_US |
dc.title | On the atmospheric neutrino oscillations, theta(13) and neutrino mass hierarchy | en_US |
dc.type | Preprint | en_US |