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On Type IIA orientifolds with flux compactifications in supersymmetric AdS vacua, we for the first time construct SU(5) models with three anti-symmetric {\bf 10} representations and without symmetric {\bf 15} representations. We show that…

High Energy Physics - Theory · Physics 2008-11-26 Ching-Ming Chen , Tianjun Li , Dimitri V. Nanopoulos

Unification of Gauge and Yukawa sectors of GUTs is obtained by searching for renormalization group invariant relations among the couplings of the both sectors which hold beyond the unification scale. This procedure singled out two…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jisuke Kubo , Myriam Mondragon , George Zoupanos

The structure of the quark and lepton masses and mixing angles provides one of the few windows we have on the underlying physics generating the \sm. In an attempt to identify the underlying symmetry group we look for the simplest gauge…

High Energy Physics - Phenomenology · Physics 2011-07-19 Luis E. Ibanez , G. G. Ross

A model based on the local gauge group SU(3)_c x SU(3)_L x U(1)_X without particles with exotic electric charges is shown to be able to provide the quark mass spectrum and their mixing, by means of universal see-saw mechanisms, avoiding a…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. Fanchiotti , C. Garcia-Canal , W. A. Ponce , .

In unified gauge theories there exist renormalization group invariant relations among gauge and Yukawa couplings that are compatible with perturbative renormalizability, which could be considered as a Gauge-Yukawa Unification. Such…

High Energy Physics - Theory · Physics 2008-02-03 Jisuke Kubo , Myriam Mondragon , George Zoupanos

Scalar leptoquarks naturally arise within unified theories, offering a promising avenue for addressing one of the most significant challenges of the Standard Model--the existence of non-zero neutrino masses. In this work, we present a…

High Energy Physics - Phenomenology · Physics 2024-05-22 Kevin Hinze , Shaikh Saad

We consider a quark-lepton symmetry model of unification of the strong and electromagnetic interactions. The model has the gauge group $SU(4)\times U(1)_{Y}$ and the minimal Higgs structure consisting of one complex quartet of scalar…

High Energy Physics - Phenomenology · Physics 2009-04-09 E. K. Loginov

We derive the singularity conditions of the N=1 generalized (general yukawa couplings and quark masses) form of hyperelliptic curves of SU(N_c) with N_f flavors. The results reproduce the known form of N=2 curves when the yukawa couplings…

High Energy Physics - Theory · Physics 2009-10-30 Takuhiro Kitao

Gauge-Yukawa Unification (GYU) is a renormalization group invariant functional relation among gauge and Yukawa couplings which holds beyond the unification point in Grand Unified Theories (GUTs). Here, GYU is obtained by requiring…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jisuke Kubo , Myriam Mondragon , George Zoupanos

I will present a simple, economic and predictive model of Yukawa structures in the context of a renormalizable SO(10) grandunification. The righthanded neutrino mass is generated radiatively. The fermions have Yukawa couplings with one 10…

High Energy Physics - Phenomenology · Physics 2007-05-23 Borut Bajc

A single mass-less fermionic field with an abelian U(1) gauge interaction (electrodynamics of a mass-less Dirac fermion) is studied by a variational method. Even without the insertion of any extra interaction the vacuum is shown to be…

High Energy Physics - Phenomenology · Physics 2009-11-10 Fabio Siringo

We explore a mechanism for radiatively generating neutrino Majorana masses in a 5 dimensional orbifold SU(5) unification model without introducing right-handed singlets. The model is non-supersymmetric and the extra dimension is…

High Energy Physics - Phenomenology · Physics 2009-11-10 We-Fu Chang , John N. Ng

We consider a minimal formulation of SO(10) Grand Unified Theory wherein all the fermion masses arise from Yukawa couplings involving one 126 and one 10 of Higgs multiplets. It has recently been recognized that such theories can explain,…

High Energy Physics - Phenomenology · Physics 2014-11-18 K. S. Babu , Cosmin Macesanu

A new Lagrangian of EW interactions without spontaneous symmetry breaking, Higgs, and Fadeev-Popov procedure has been constructed. It consists of three parts: $SU(2)_L\times U(1)$ gauge fields, massive fermion fields, and their…

High Energy Physics - Phenomenology · Physics 2009-09-28 Bing An Li

We study supersymmetric unified models with three fermion generations based on the gauge group $SO(10)$ and require Gauge-Yukawa Unification, i.e., a renormalization group invariant functional relationship among the gauge and Yukawa…

High Energy Physics - Phenomenology · Physics 2011-01-27 Jisuke Kubo , Myriam Mondragon , Shigeyuki Shoda , George Zoupanos

We present a new mechanism for gluino mass generation in models of dynamical supersymmetry breaking. The mechanism requires two colored chiral superfields which feel a nonabelian gauge interaction such that a fermion condensate is formed at…

High Energy Physics - Phenomenology · Physics 2016-08-24 Bogdan A. Dobrescu

The gauge symmetry of the Standard Model is SU(3)_c x SU(2)_L x U(1)_Y for unknown reasons. One aspect that can be addressed is the low dimensionality of all its subgroups. Why not much larger groups like SU(7), or for that matter, SP(38)…

High Energy Physics - Phenomenology · Physics 2016-12-30 Guillermo Garcia Fernandez , Jesus Guerrero Rojas , Felipe J. Llanes-Estrada

Gauge-Yukawa Unification (GYU) is obtained in GUTs by searching for renormalization group invariant relations among gauge and Yukawa couplings beyond the unification scale. Of particular interest are two supersymmetric GUTs, the finite and…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Kubo , M. Mondragon , G. Zoupanos

We consider a field theoretical model where a SU(2) fermion doublet, subjected to non-Abelian gauge interactions, is also coupled to a complex scalar field doublet via a Yukawa and an irrelevant Wilson-like term. Despite the presence of…

We calculate gaugino and meson condensates in N=1 SQCD theory with SU(N_c) gauge group and N_f < 2N_c matter flavours, by deforming the pure N=2 Super-Yang-Mills plus fundamental matter action with a mass term for the adjoint scalar…

High Energy Physics - Theory · Physics 2007-05-23 Michael Chesterman