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      Towards a realistic model of quarks and leptons, leptonic CP violation and neutrinoless \(\beta\beta\)-decay

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          Abstract

          In order to explain the fermion masses and mixings naturally, we introduce a specific flavor symmetry and mass suppression pattern that constrain the flavor structure of the fermion Yukawa couplings. Our model describes why the hierarchy of neutrino masses is milder than the hierarchy of charged fermion masses in terms of successive powers of flavon fields. We investigate CP violation and neutrinoless double beta (\(0\nu\beta\beta\)) decay, and show how they can be predicted and constrained in our model by present and upcoming experimental data. Our model predicts that the atmospheric neutrino mixing angle \(\theta_{23}\) should be within \(\sim1^{\circ}\) of \(45^\circ\) for the normal neutrino mass ordering (NO), and between \(\sim4^\circ\) and \(\sim8^\circ\) degrees away from \(45^\circ\) (in either direction) for the inverted neutrino mass ordering (IO). For both NO and IO, our model predicts that a \(0\nu\beta\beta\) Majorana mass in the limited range \(0.035 \text{eV}<|m_{ee}|\lesssim0.15\) eV, which can be tested in current experiments. Moreover, our model can successfully accommodate flavorless leptogenesis as the mechanism to generate the baryon asymmetry in the Universe, provided the neutrino mass ordering is normal, \(|m_{ee}|\simeq0.072\pm0.012\) eV, and either \(\theta_{23}\simeq44^{\circ}\) and the Dirac CP-violating phase \(\delta_{CP}\simeq20^{\circ}\) or \(60^{\circ}\), or \(\theta_{23}\simeq46^{\circ}\) and \(\delta_{CP} \simeq205^{\circ}\) or \(245^{\circ}\).

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          Most cited references2

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          The Seesaw Mechanism in Quark-Lepton Complementarity

          We systematically construct realistic mass matrices for the type-I seesaw mechanism out of more than 20 trillion possibilities. We use only very generic assumptions from extended quark-lepton complementarity, i.e., the leptonic mixing angles between flavor and mass eigenstates are either maximal, or parameterized by a single small quantity epsilon that is of the order of the Cabibbo angle epsilon theta_C. The small quantity epsilon also describes all fermion mass hierarchies. We show that special cases often considered in the literature, such as having a symmetric Dirac mass matrix or small mixing among charged leptons, constitute only a tiny fraction of our possibilities. Moreover, we find that in most cases the spectrum of right-handed neutrino masses is only mildly hierarchical. As a result, we provide for the charged leptons and neutrinos a selected list of 1981 qualitatively different Yukawa coupling matrices (or textures) that are parameterized by the Cabibbo angle and allow for a perfect fit to current data. In addition, we also briefly show how the textures could be generated in explicit models from flavor symmetries.
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            Simple renormalizable flavor symmetry for neutrino oscillations

            The recent measurement of a non-zero neutrino mixing angle \(\theta_{13}\) requires a modification of the tri-bimaximal mixing pattern that predicts a zero value for it. We propose a new neutrino mixing pattern based on a spontaneously-broken \(A_{4}\) flavor symmetry and a type-I seesaw mechanism. Our model allows for approximate tri-bimaximal mixing and non-zero \(\theta_{13}\), and contains a natural way to implement low and high energy CP violation in neutrino oscillations, and leptogenesis with a renormalizable Lagrangian. Both normal and inverted mass hierarchies are permitted within \(3\sigma\) experimental bounds, with the prediction of small (large) deviations from maximality in the atmospheric mixing angle for the normal (inverted) case. Interestingly, we show that the inverted case is excluded by the global analysis in \(1\sigma\) experimental bounds, while the most recent MINOS data seem to favor the inverted case. Our model make predictions for the Dirac CP phase in the normal and inverted hierarchies, which can be tested in near-future neutrino oscillation experiments. Our model also predicts the effective mass \(|m_{ee}|\) measurable in neutrinoless double beta decay to be in the range \(0.04\lesssim |m_{ee}| \lesssim 0.15\) eV for the normal hierarchy and \(0.06\lesssim |m_{ee}| \lesssim 0.11\) eV for the inverted hierarchy, both of which are within the sensitivity of the next generation experiments.

              Author and article information

              Journal
              02 February 2014
              2014-12-08
              Article
              10.1103/PhysRevD.91.013007
              1402.0150
              fbf05379-20ec-4e03-9338-b3266fac562e

              http://arxiv.org/licenses/nonexclusive-distrib/1.0/

              History
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              41 pages and 13 figures, references added, version to appear in PRD; the model is changed slightly without corrupting the numerical results
              hep-ph

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