Abstract:Following recent results from the SNO solar neutrino experiment and the K2K long-baseline neutrino experiment, the combined existing data on neutrino oscillations now point strongly to a specific form for the lepton mixing matrix, with effective bimaximal mixing of ν µ and ν τ at the atmospheric scale and effective trimaximal mixing for ν e with ν µ and ν τ at the solar scale (hence 'tri-bimaximal' mixing). We give simple mass-matrices leading to tri-bimaximal mixing, and discuss its relation to the Fritzsch-X… Show more
“…We emphasise that, unlike [14], tri-bimaximal mixing in the neutrino sector is merely a staging point in our considerations, and the final form of the lepton mixing matrix, after charged lepton mixing angles have been taken into account, will not have the tri-bimaximal form. We therefore refer to this approach as tri-bimaximal complementarity to distinguish it from the usual tri-bimaximal neutrino mixing.…”
We show how the neutrino mixing angles and oscillation phase can be predicted from tri-bimaximal neutrino mixing, corrected by charged lepton mixing angles which are related to quark mixing angles via quark-lepton unification. The tribimaximal neutrino mixing can naturally originate from the see-saw mechanism via constrained sequential dominance (CSD), where CSD can result from the vacuum alignment of a non-Abelian family symmetry such as SO(3). We construct a realistic model of quark and lepton masses and mixings based on SO (3) These predictions can all be tested by future high precision neutrino oscillation experiments, thereby probing the nature of high energy quark-lepton unification.
“…We emphasise that, unlike [14], tri-bimaximal mixing in the neutrino sector is merely a staging point in our considerations, and the final form of the lepton mixing matrix, after charged lepton mixing angles have been taken into account, will not have the tri-bimaximal form. We therefore refer to this approach as tri-bimaximal complementarity to distinguish it from the usual tri-bimaximal neutrino mixing.…”
We show how the neutrino mixing angles and oscillation phase can be predicted from tri-bimaximal neutrino mixing, corrected by charged lepton mixing angles which are related to quark mixing angles via quark-lepton unification. The tribimaximal neutrino mixing can naturally originate from the see-saw mechanism via constrained sequential dominance (CSD), where CSD can result from the vacuum alignment of a non-Abelian family symmetry such as SO(3). We construct a realistic model of quark and lepton masses and mixings based on SO (3) These predictions can all be tested by future high precision neutrino oscillation experiments, thereby probing the nature of high energy quark-lepton unification.
“…Indeed, we find that with appropriate choice of representations, the tri-bimaximal mixing pattern [18] characteristic of the A 4 symmetry can be reproduced by the leading order operators. Higher order terms can result in non-zero θ 13 , while maintaining the predictions for θ 12 , θ 23 within the experimentally allowed range.…”
Section: Introductionmentioning
confidence: 87%
“…We work in the basis of diagonal charged leptons which is obtained by performing the rotation on the entire left-handed doublet with V. Then, the light neutrino Majorana mass matrix is diagonalized by the Harrison-PerkinsScott (HPS) matrix [18] 14) corresponding to θ 13 = 0, sin 2 (2θ 12 ) = 8/9 and θ 23 = π/4. This tri-bimaximal mixing matrix is very close to the the best fit obtained from present oscillation data.…”
In order to explain the non-hierarchical neutrino mixing angles and the absence of lepton flavor violating processes in the context of warped extra dimensions one needs to introduce bulk flavor symmetries. We present a simple model of lepton masses and mixings in RS models based on the A 4 non-abelian discrete symmetry. The virtues of this choice are: (i) the natural appearance of the tri-bimaximal mixing pattern; (ii) the complete absence of tree-level flavor violations in the neutral sector; (iii) the absence of flavor gauge bosons; (iv) the hierarchies in the charged lepton masses are explained via wave-function overlaps. We present the minimal field content and symmetry breaking pattern necessary to obtain a successful model of this type. The bounds from electroweak precision measurements allow the KK mass scale to be as low as ∼ 3 TeV. Tree-level lepton flavor violation is absent in this model, while the loop induced µ → eγ branching fraction is safely below the experimental bound.
“…One guiding principle for precision measurements of neutrino oscillations should be the ability to provide unambiguous tests of these relations. An example is given by the tri-bimaximal mixing pattern (sin 2 θ 23 = 1/2, sin 2 θ 12 = 1/3, and sin 2 θ 13 = 0) [28]; a popular, zeroth-order ansatz that guides theoretical research in neutrino flavour. Different models make different predictions regarding deviations from this ansatz, which are usually small and proportional to some other small parameters in flavour physics.…”
Section: The Physics Case For Advanced Neutrino Experimentsmentioning
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