288 research outputs found

    Effect of CP-Odd Planck Scale Induced Operators on the Majoron Scale

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    Definitions of the control sequences included, but no other changes.Comment: 6 pages, Tex (hep-ph/9305259

    Decay of the Z Boson into Scalar Particles

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    In extensions of the standard model, light scalar particles are often possible because of symmetry considerations. We study the decay of the Z boson into such particles. In particular, we consider for illustration the scalar sector of a recently proposed model of the 17-keV neutrino which satisfies all laboratory, astrophysical, and cosmological constraints.Comment: 11 pages (2 figures, not included) (Revised, Oct 1992). Some equations have been corrected and 1 figure has been eliminate

    Spontaneous breaking of a global symmetry in a 331 model

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    In a 331 model in which the lepton masses arise from a scalar sextet it is possible to break spontaneously a global symmetry implying in a pseudoscalar majoron-like Goldstone boson. This majoron does not mix with any other scalar fields and for this reason it does not couple, at the tree level, neither to the charged leptons nor to the quarks. Moreover, its interaction with neutrinos is diagonal. We also argue that there is a set of the parameters in which that the model can be consistent with the invisible Z^0-width and that heavy neutrinos can decay sufficiently rapid by majoron emission having a lifetime shorter than the age of the universe.Comment: RevTex, 10 pages, one .eps figur

    Light-Heavy Symmetry: Geometric Mass Hierarchy for Three Families

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    The Universal Seesaw pattern coupled with a Light↔\leftrightarrowHeavy symmetry principle leads to the Diophantine equation N=∑i=1Nni\displaystyle N = \sum_{i=1}^Nn_i, where ni≄0n_i\geq 0 and distinct. Its unique non-trivial solution (3=0+1+2)(3=0+1+2) gives rise to the geometric mass hierarchy mWm_W, mWÏ”m_W\epsilon, mWÏ”2m_W\epsilon^2 for N=3N=3 fermion families. This is realized in a model where the hybrid (yet Up↔\leftrightarrowDown symmetric) quark mass relations mdmt≈mc2↔mumb≈ms2m_d m_t \approx m_c^2\leftrightarrow m_u m_b \approx m_s^2 play a crucial role in expressing the CKM mixings in terms of simple mass ratios, notably sin⁥ΞC≈mcmb\sin\theta_C \approx {m_c\over m_b}.Comment: 12 pages, no figures, Revtex fil

    Radiative Seesaw Mechanism at Weak Scale

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    We investigate an alternative seesaw mechanism for neutrino mass generation. Neutrino mass is generated at loop level but the basic concept of usual seesaw mechanism is kept. One simple model is constructed to show how this mechanism is realized. The applications of this seesaw mechanism at weak scale to cosmology and neutrino physics are discussed.Comment: 12 Pages, latex, no figure
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