Abstract:Abstract:We analyse the interplay of generalised CP transformations and the nonAbelian discrete group T and use the semi-direct product G f = T H CP , as family symmetry acting in the lepton sector. The family symmetry is shown to be spontaneously broken in a geometrical manner. In the resulting flavour model, naturally small Majorana neutrino masses for the light active neutrinos are obtained through the type I see-saw mechanism. The known masses of the charged leptons, lepton mixing angles and the two neutri… Show more
“…The existence of massive neutrinos at the eV scale can be probed in β-decay experiments [219][220][221][222][223][224][225] and in neutrinoless double-β decay experiments [13,106,176,[226][227][228][229][230][231][232][233][234].…”
Section: β Decay and Neutrinoless Double-β Decaymentioning
Abstract. The theory and phenomenology of light sterile neutrinos at the eV mass scale is reviewed. The reactor, Gallium and LSND anomalies are briefly described and interpreted as indications of the existence of short-baseline oscillations which require the existence of light sterile neutrinos. The global fits of short-baseline oscillation data in 3+1 and 3+2 schemes are discussed, together with the implications for β-decay and neutrinoless double-β decay. The cosmological effects of light sterile neutrinos are briefly reviewed and the implications of existing cosmological data are discussed. The review concludes with a summary of future perspectives.
“…The existence of massive neutrinos at the eV scale can be probed in β-decay experiments [219][220][221][222][223][224][225] and in neutrinoless double-β decay experiments [13,106,176,[226][227][228][229][230][231][232][233][234].…”
Section: β Decay and Neutrinoless Double-β Decaymentioning
Abstract. The theory and phenomenology of light sterile neutrinos at the eV mass scale is reviewed. The reactor, Gallium and LSND anomalies are briefly described and interpreted as indications of the existence of short-baseline oscillations which require the existence of light sterile neutrinos. The global fits of short-baseline oscillation data in 3+1 and 3+2 schemes are discussed, together with the implications for β-decay and neutrinoless double-β decay. The cosmological effects of light sterile neutrinos are briefly reviewed and the implications of existing cosmological data are discussed. The review concludes with a summary of future perspectives.
“…In the field of discrete flavour models, this indication translated into looking, for the first time, for approaches and/or contexts where, besides the mixing angles, also the lepton phase(s) were predicted: new models were presented with the CP symmetry as part of the full flavour symmetry [94][95][96][97][98][99][100]; studies on the mixing patterns and their modifications to provide realistic descriptions of oscillation data were performed [101][102][103][104]; an intense activity was dedicated to investigate sum rules involving neutrino masses, mixing angles and δ CP [102][103][104][105][106][107][108][109].…”
The Minimal Lepton Flavour Violation (MLFV) framework is discussed after the recent indication for CP violation in the leptonic sector. Among the three distinct versions of MLFV, the one with degenerate right-handed neutrinos will be disfavoured, if this indication is confirmed. The predictions for leptonic radiative rare decays and muon conversion in nuclei are analysed, identifying strategies to disentangle the different MLFV scenarios. The claim that the present anomalies in the semi-leptonic B-meson decays can be explained within the MLFV context is critically re-examined concluding that such an explanation is not compatible with the present bounds from purely leptonic processes.
“…The invariance of the light neutrino mass matrix under µ − τ reflection in the charged lepton diagonal basis leads to maximal atmospheric mixing angle θ 23 and maximal Dirac CP phase δ CP with δ CP = ±π/2 [33][34][35][36][37][38][39]. The phenomenological implications of the generalized CP symmetry has been analyzed within the context of popular A 4 [40], S 4 [30,[41][42][43][44] and T [45] family symmetries. By breaking the full symmetry down to Z 2 ×CP in the neutrino sector, the TM 1 and TM 2 mixing patterns in which the first and the second columns of the tri-bimaximal mixing is kept respectively, can be exactly produced.…”
The lepton flavor mixing matrix having one row or one column in common with the bimaximal mixing up to permutations is still compatible with the present neutrino oscillation data. We provide a thorough exploration of generating such a mixing matrix from S 4 family symmetry and generalized CP symmetry H CP . Supposing that S 4 H CP is broken down to Z ST 2 SU 2 × H ν CP in the neutrino sector and Z T ST 2 U
4H l CP in the charged lepton sector, one column of the PMNS matrix would be of the form 1/2, 1/ √ 2, 1/2 T up to permutations, both Dirac CP phase and Majorana CP phases are trivial to accommodate the observed lepton mixing angles. The phenomenological implications of the remnant symmetry K× H ν CP in the neutrino sector and Z SU 2 × H l CP in the charged lepton sector are studied. One row of PMNS matrix is determined to be 1/2, 1/2, −i/ √ 2 , and all the three leptonic CP phases can only be trivial to fit the measured values of the mixing angles. Two models based on S 4 family symmetry and generalized CP are constructed to implement these model independent predictions enforced by remnant symmetry. The correct mass hierarchy among the charged leptons is achieved. The vacuum alignment and higher order corrections are discussed.
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