438 research outputs found

    Non-Abelian Discrete Flavor Symmetries on Orbifolds

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    We study non-Abelian flavor symmetries on orbifolds, S1/Z2S^1/Z_2 and T2/Z3T^2/Z_3. Our extra dimensional models realize DND_N, Σ(2N2)\Sigma(2N^2), Δ(3N2)\Delta(3N^2) and Δ(6N2)\Delta(6N^2) including A4A_4 and S4S_4. In addition, one can also realize their subgroups such as QNQ_N, T7T_7, etc. The S3S_3 flavor symmetry can be realized on both S1/Z2S^1/Z_2 and T2/Z3T^2/Z_3 orbifolds.Comment: 16 page

    Bilinear R-parity violation with flavor symmetry

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    Bilinear R-parity violation (BRPV) provides the simplest intrinsically supersymmetric neutrino mass generation scheme. While neutrino mixing parameters can be probed in high energy accelerators, they are unfortunately not predicted by the theory. Here we propose a model based on the discrete flavor symmetry A4A_4 with a single R-parity violating parameter, leading to (i) correct Cabbibo mixing given by the Gatto-Sartori-Tonin formula, and a successful unification-like b-tau mass relation, and (ii) a correlation between the lepton mixing angles θ13\theta_{13} and θ23\theta_{23} in agreement with recent neutrino oscillation data, as well as a (nearly) massless neutrino, leading to absence of neutrinoless double beta decay.Comment: 16 pages, 3 figures. Extended version, as published in JHE

    Z_2 Symmetry Prediction for the Leptonic Dirac CP Phase

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    Model-independent consequences of applying a generalized hidden horizontal Z_2 symmetry to the neutrino mass matrix are explored. The Dirac CP phase delta_D can be expressed in terms of the three mixing angles as 4 c_a s_a c_s s_s s_x cos delta_D = (s^2_s - c^2_s s^2_x) (c^2_a - s^2_a) where the s_i, c_i are sines and cosines of the atmospheric, solar, and reactor angles. This relation is independent of neutrino masses and whether neutrinos are Dirac- or Majorana-type. Given the present constraints on the angles, delta_D is constrained to be almost maximal, a result which can be explored in experiments such as NOvA and T2K. The Majorana CP phases do not receive any constraint and are thus model-dependent. Also a distribution of theta_x with a lower limit is obtained without specifying delta_D.Comment: 5 pages, 4 figures; Condensed version or PLB with references added; for more details see the previous versio

    Direct and Indirect Detection of Dark Matter in D6 Flavor Symmetric Model

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    We study a fermionic dark matter in a non-supersymmetric extension of the standard model with a family symmetry based on D6xZ2xZ2. In our model, the final state of the dark matter annihilation is determined to be e+ e- by the flavor symmetry, which is consistent with the PAMELA result. At first, we show that our dark matter mass should be within the range of 230 GeV - 750 GeV in the WMAP analysis combined with mu to e gamma constraint. Moreover we simultaneously explain the experiments of direct and indirect detection, by simply adding a gauge and D6 singlet real scalar field. In the direct detection experiments, we show that the lighter dark matter mass ~ 230 GeV and the lighter standard model Higgs boson ~ 115 GeV is in favor of the observed bounds reported by CDMS II and XENON100. In the indirect detection experiments, we explain the positron excess reported by PAMELA through the Breit-Wigner enhancement mechanism. We also show that our model is consistent with no antiproton excess suggested by PAMELA.Comment: 20 pages, 9 figures, 2 tables, accepted version for publication in European Physical Journal

    Electron and Muon g−2g-2 Contributions from the T′T' Higgs Sector

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    We study the experimental constraints from electron and muon g−2g-2 factors on the Higgs masses and Yukawa couplings in the T′T' model, and thereby show that the discrepancy between the standard model prediction and experimental value of muon anomalous g−2g-2 factor can be easily accommodated.Comment: 7 pages, slightly modified and new references adde

    Repressing Anarchy in Neutrino Mass Textures

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    The recent results that θ13\theta_{13} is relatively large, of the order of the previous upper bound, and the indications of a sizable deviation of θ23\theta_{23} from the maximal value are in agreement with the predictions of Anarchy in the lepton sector. The quark and charged lepton hierarchies can then be reproduced in a SU(5) GUT context by attributing non-vanishing U(1)FNU(1)_{FN} charges, different for each family, only to the SU(5) tenplet states. The fact that the observed mass hierarchies are stronger for up quarks than for down quarks and charged leptons supports this idea. As discussed in the past, in the flexible context of SU(5)⊗U(1)FNSU(5)\otimes U(1)_{FN}, different patterns of charges can be adopted going from Anarchy to various types of hierarchy. We revisit this approach by also considering new models and we compare all versions to the present data. As a result we confirm that, by relaxing the extreme ansatz of equal U(1)FNU(1)_{FN} charges for all SU(5) pentaplets and singlets, better agreement with the data than for Anarchy is obtained without increasing the model complexity. We also present the distributions obtained in the different models for the Dirac CP-violating phase. Finally we discuss the relative merits of these simple models.Comment: v1: 12 pages, 3 figures; v2: 13 pages, 3 figures, text improved, matches version accepted for publication; v3: submitted to add an acknowledgment to a networ

    Strain Relaxation Mechanisms and Local Structural Changes in Si_{1-x}$Ge_{x} Alloys

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    In this work, we address issues pertinent to the understanding of the structural and electronic properties of Si_{1-x} Ge_{x}alloys, namely, (i) how does the lattice constant mismatch between bulk Si and bulk Ge manifests itself in the alloy system? and (ii) what are the relevant strain release mechanisms? To provide answers to these questions, we have carried out an in-depth study of the changes in the local geometric and electronic structures arising from the strain relaxation in Si_{1-x} Ge_{x} alloys using an ab initio molecular dynamics scheme. The optimized lattice constant, while exhibiting a general trend of linear dependence on the composition (Vegard's law), shows a negative deviation from Vegard's law in the vicinity of x=0.5. We delineate the mechanisms responsible for each one of the above features. We show that the radial-strain relaxation through bond stretching is responsible for the overall trend of linear dependence of the lattice constant on the composition. On the other hand, the negative deviation from Vegard's law is shown to arise from the angular-strain relaxation.Comment: 21 pages, 7 figure

    A Note on Embedding Nonabelian Finite Flavor Groups in Continuous Groups

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    A nonabelian finite flavor group G⊂SO(3)G \subset SO(3) can have double covering G′⊂SU(2)G^{'} \subset SU(2) such that G⊄G′G \not\subset G^{'}. This situation is not contradictory, but quite natural, and we give explicit examples such as G=Dn,G′=Q2nG=D_n, G^{'}=Q_{2n} and G=T,G′=T′G=T, G^{'}=T^{'}. This observation can be crucial in particle theory model building.Comment: Example of application adde

    Accidental stability of dark matter

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    We propose that dark matter is stable as a consequence of an accidental Z2 that results from a flavour-symmetry group which is the double-cover group of the symmetry group of one of the regular geometric solids. Although model-dependent, the phenomenology resembles that of a generic Higgs portal dark matter scheme.Comment: 12 pages, final version, published in JHE

    Search for Supernova Relic Neutrinos at Super-Kamiokande

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    A search for the relic neutrinos from all past core-collapse supernovae was conducted using 1496 days of data from the Super-Kamiokande detector. This analysis looked for electron-type anti-neutrinos that had produced a positron with an energy greater than 18 MeV. In the absence of a signal, 90% C.L. upper limits on the total flux were set for several theoretical models; these limits ranged from 20 to 130 nu_e bar cm^-2 s^-1. Additionally, an upper bound of 1.2 nu_e bar cm^-2 s^-1 was set for the supernova relic neutrino flux in the energy region E_nu > 19.3 MeV.Comment: 4 pages, 2 figures. Submitted to Physical Review Letters. New version includes corrections to Figure 1. Also, text has been shortened to conform with the space limitations of PR
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