49,321 research outputs found

    A Highly Predictive Ansatz for Leptonic Mixing and CP Violation

    Full text link
    We suggest a simple highly predictive ansatz for charged lepton and light neutrino mass matrices, based on the assumption of universality of Yukawa couplings. Using as input the charged lepton masses and light neutrino masses, the six parameters characterizing the leptonic mixing matrix VPMNSV_{PMNS}, are predicted in terms of a single phase ϕ\phi, which takes a value around ϕ=π2\phi={\frac{\pi}{2}}. Correlations among variuos physical quantities are obtained, in particular V13PMNSV^{PMNS}_{13} is predicted as a function of Δm212{\Delta}m^2_{21}, Δm312{\Delta}m^2_{31} and sin2(θsol)\sin^2(\theta_{sol}), and restricted to the range 0.167<V13PMNS<0.1790.167<|V^{PMNS}_{13}|<0.179.Comment: 9 pages, 4 figure

    Leptonic Invariants, Neutrino Mass-Ordering and the Octant of θ23\theta_{23}

    Full text link
    We point out that leptonic weak-basis invariants are an important tool for the study of the properties of lepton flavour models. In particular, we show that appropriately chosen invariants can give a clear indication of whether a particular lepton flavour model favours normal or inverted hierarchy for neutrino masses and what is the octant of θ23\theta_{23}. These invariants can be evaluated in any conveniently chosen weak-basis and can also be expressed in terms of neutrino masses, charged lepton masses, mixing angles and CP violation phases.Comment: 10 pages, no figure

    Non-Factorizable Phases, Yukawa Textures and the Size of sin (2 beta)

    Full text link
    We emphasize the crucial r\^ ole played by non-factorizable phases in the analysis of the Yukawa flavour structure performed in weak bases with Hermitian mass matrices and with vanishing (1,1)(1,1) entries. We show that non-factorizable phases are important in order to generate a sufficiently large sin2β\sin 2 \beta . A method is suggested to reconstruct the flavour structure of Yukawa couplings from input experimental data both in this Hermitian basis and in a non-Hermitian basis with a maximal number of texture zeros. The corresponding Froggatt--Nielsen patterns are presented in both cases.Comment: 15 pages, 3 figure

    Vortex solutions of the Lifshitz-Chern-Simons theory

    Get PDF
    We study vortex-like solutions to the Lifshitz-Chern-Simons theory. We find that such solutions exists and have a logarithmically divergent energy, which suggests that a Kostelitz-Thouless transition may occur, in which voxtex-antivortex pairs are created above a critical temperature. Following a suggestion made by Callan and Wilzcek for the global U(1) scalar field model, we study vortex solutions of the Lifshitz-Chern-Simons model formulated on the hyperbolic plane, finding that, as expected, the resulting configurations have finite energy. For completeness, we also explore Lifshitz-Chern-Simons vortex solutions on the sphere.Comment: Published version, added appendix on electromagnetic duality in Lifshitz system

    Quasidegeneracy of Majorana Neutrinos and the Origin of Large Leptonic Mixing

    Full text link
    We propose that the observed large leptonic mixing may just reflect a quasidegeneracy of three Majorana neutrinos. The limit of exact degeneracy of Majorana neutrinos is not trivial, as leptonic mixing and even CP violation may occur. We conjecture that the smallness of U13|U_{13}|, when compared to the other elements of UPMNSU_{PMNS}, may just reflect the fact that, in the limit of exact mass degeneracy, the leptonic mixing matrix necessarily has a vanishing element. We show that the lifting of the mass degeneracy can lead to the measured value of U13|U_{13}| while at the same time accommodating the observed solar and atmospheric mixing angles. In the scenario we consider for the breaking of the mass degeneracy there is only one CP violating phase, already present in the limit of exact degeneracy, which upon the lifting of the degeneracy generates both Majorana and Dirac-type CP violation in the leptonic sector. We analyse some of the correlations among physical observables and point out that in most of the cases considered, the implied strength of leptonic Dirac-type CP violation is large enough to be detected in the next round of experiments.Comment: 16 pages, 4 figures. Matches published version, references added, improved discussion, results unchange

    What if the Masses of the First Two Quark Families are not Generated by the Standard Higgs?

    Full text link
    We point out that, in the context of the SM, V132+V232|V^2_{13}| + | V^2_{23}| is expected to be large, of order one. The fact that V132+V2321.6×103|V^2_{13}| + |V^2_{23}| \approx 1.6 \times 10^{-3} motivates the introduction of a symmetry S which leads to VCKM=1 ⁣ ⁣ ⁣IV_{CKM} ={1\>\!\!\!\mathrm{I}} , with only the third generation of quarks acquiring mass. We consider two scenarios for generating the mass of the first two quark generations and full quark mixing. One consists of the introduction of a second Higgs doublet which is neutral under S. The second scenario consists of assuming New Physics at a high energy scale , contributing to the masses of light quark generations, in an effective field theory approach. This last scenario leads to couplings of the Higgs particle to sss\overline s and ccc \overline c which are significantly enhanced with respect to those of the SM. In both schemes, one has scalar-mediated flavour- changing neutral currents which are naturally suppressed. Flavour violating top decays are predicted in the second scenario at the level \mbox{Br} (t \rightarrow h c ) \geq 5\times 10^{-5}.Comment: 11 pages, 1 figur

    Non(anti)commutative superspace with coordinate-dependent deformation

    Full text link
    We consider non(anti)commutative superspace with coordinate dependent deformation parameters CαβC^{\alpha\beta}. We show that a chiral N=1/2{\cal N}=1/2 supersymmetry can be defined and that chiral and antichiral superfields are still closed under the Moyal-Weyl associative product implementing the deformation. A consistent N=1/2{\cal N}=1/2 Super Yang-Mills deformed theory can be constructed provided CαβC^{\alpha\beta} satisfies a suitable condition which can be connected with the graviphoton background at the origin of the deformation. After adding matter we also discuss the Konishi anomaly and the gluino condensation.Comment: References added. Accepted for publication in PR
    corecore