13 research outputs found

    Renormalization Group Effects on the Mass Relation Predicted by the Standard Model with Generalized Covariant Derivatives

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    Renormalization group analysis is made on the relation mH2mtm_{\rm H} \simeq \sqrt{2}m_t for masses of the top quark and the Higgs boson, which is predicted by the standard model based on generalized covariant derivatives with gauge and Higgs fields. This relation is a low energy manifestation of a tree level constraint which holds among the quartic Higgs self-coupling constant and the Yukawa coupling constants at a certain high energy scale μ0\mu_0. With the renormalization group equation at one-loop level, the evolution of the constraint is calculated from μ0\mu_0 down to the low energy region around the observed top quark mass. The result of analysis shows that the Higgs boson mass is in mtmH2mtm_t \lesssim m_{\rm H} \lesssim \sqrt{2}m_t for a wide range of the energy scale μ0mt\mu_0 \gtrsim m_t and it approaches to 177 GeV (mt\approx m_t) for large values of μ0\mu_0.Comment: 13 pages, LaTeX, no figure

    Universal Seesaw Mechanism with Universal Strength for Yukawa Couplings

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    Hypotheses of the universal seesaw mechanism and the {\it universal strength for Yukawa couplings} are applied to explain one possible origin of quasi-democratic mass matrices of a special type in a left-right symmetric model with the gauge group SU(3)c×SU(2)L×SU(2)R×U(1)SU(3)_c\times SU(2)_L\times SU(2)_R\times U(1). Two kinds of Higgs doublets are postulated to mediate scalar interactions between the ii-th generation of light fermion doublets and the jj-th generation of heavy fermion singlets with relative Yukawa coupling constants of the exponential form eiϕije^{i\phi_{ij}}, where ϕij\phi_{ij} are real phase constants. The lowest seesaw approximation results effectively in self-adjoint mass matrices which are quasi-democratic and have the same diagonal elements. A set of values for the parameters ϕij\phi_{ij} is found which reproduces the present experimental data for the absolute values of the CKM matrix elements, the Jarlskog parameter and the Wolfenstein parameters.Comment: Latex, 16 pages, no figure

    Flavor Changing Neutral Currents in Universal Seesaw Model

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    Universal Seesaw Mechanism for Quarks and Leptons

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