1996


    US-96-10
    November 1996
    (hep-ph/9612322)
    Prog.Theor.Phys. 97, 459 (1997)

    Analytical Expressions of Masses and Mixings in a Democratic Seesaw Mass Matrix Model

    Yoshio Koide and Hideo Fusaoka

    Abstract

    On the basis of a seesaw-type mass matrix model $M_f\simeq m_L M_F^{-1} m_R$ for quarks and leptons $f$, analytical expressions of the masses and mixings of the fermions $f$ are investigated. Here, the matrices $m_L$ and $m_R$ are common to all $f$ (up- and down-; quarks and leptons), and the matrix $M_F$ characterizing the heavy fermion sector has the form [(unit matrix)+ (democratic-type matrix)]. An application to the quark sectors is discussed.
    Latex file

    US-96-09
    November 1996
    (hep-ph/9701261)

    Flavor-Changing Neutral Currents Induced by the Democratic Seesaw Mass Matrix

    Yoshio Koide

    Abstract

    Flavor-changing neutral currents (FCNC) are studied on the basis of a ``democratic seesaw" mass matrix model, which yields a singular enhancement of the top-quark mass $m_t$ and can give reasonable quark masses and CKM matrix elements. The most exciting aspect of the model is that the structure of the $6 \times 6$ right-handed fermion mixing matrix in the up-quark sector, $U^R_u$, shows an abnormal structure in contrast to that of $U^L_u$. This causes characteristic effects on the right-handed FCNC concerned with top quark. A single top-quark production at future $e^+ e^-$ colliders, $e^+ + e^- \rightarrow Z_R \rightarrow t + \overline{c}$ ($\overline{t}+c$), is discussed.
    Latex file

    US-96-05
    September 1996
    (hep-th/9609014)

    New Algorithm for Tensor Calculation in Field Theories

    Shoichi ICHINOSE

    Abstract

    Tensor calculation of suffix-contraction is carried out by a C-program. Tensors are represented graphically, and the algorithm makes use of the topology of graphs. Classical and quantum gravity, in the weak-field perturbative approach, is a special interest. Examples of the leading order calculation of some general invariants such as $R_{\mu\nu\lambda\sigma} R^{\mu\nu\lambda\sigma}$~ are given. Application to Weyl anomaly calculation is commented.

    US -96 - 04
    March 1996
    (hep-ph/9603376)
    Mod.Phys.Lett. A11, 2849 (1996)

    Neutrino Mixing in a Democratic-Seesaw-Mass-Matrix Model

    Yoshio Koide

    Abstract

    On the basis of a seesaw-type mass matrix model for quarks and leptons, $M_f \simeq m_L M_F^{-1} m_R$, where $m_L\propto m_R$ are universal for $f=u,d,\nu$ and $e$ (up-quark-, down-quark-, neutrino- and charged lepton-sectors), and $M_F$ has a form [(unit matrix)+(democratic-type matrix)], neutrino masses and mixings are investigated. It is tried to understand a large $\nu_\mu$-$\nu_\tau$ mixing, i.e., $\sin^2 2\theta_{23}\sim 1$, with $m_{\nu 1} \ll m_{\nu 2} \sim m_{\nu 3}$, which has been suggested by the atmospheric neutrino data.
    Latex file (including figures)
    Latex file only

    US-96-03
    September 1996
    (hep-th/9609013)

    Weak Field Expansion of Gravity and Graphical Representation

    Shoichi ICHINOSE and Noriaki IKEDA

    Abstract

    We introduce a graphical representation for a global SO(n) tensor $\partial_\mu\partial_\nu h_{\alpha\beta}$, which generally appears in the perturbative approach of gravity around the flat space: $g_{\mu\nu}=\delta_{\mu\nu}+h_{\mu\nu}$. We systematically construct global SO(n) invariants. Independence and completeness of those invariants are shown by taking examples of $\partial\partial h$-, and $ (\partial\partial h)^2$- invariants. They are classified graphically. Indices which characterize all independent invariants (or graphs) are given. We apply the results to general invariants with dimension $(Mass)^4$~ and the Gauss-Bonnet identity in 4-dim gravity.

  • US - 96 - 02 and AMU - 96 - 01
    February 1996
    (hep-ph/9602303)

    A Democratic Seesaw Quark Mass Matrix Related to the Charged Lepton Masses

    Yoshio Koide and Hideo Fusaoka
    Latex file

    Abstract

    We investigate a seesaw type mass matrix $M_f\simeq m_L M_F^{-1} m_R$ for quarks and leptons, $f$, under the assumptions that the matrices $m_L$ and $m_R$ have common structures for the quarks and leptons, and that the matrix $M_F$ characterizing the heavy fermion sector has the form [(unit matrix)+ (democratic-type matrix)]. We obtain well-satisfied relations for quark masses and mixings related to the charged lepton masses.