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We present an $E_6$ Grand Unified model with a realistic pattern of fermion masses. All standard model fermions are unified in three fundamental 27-plets (i.e. supersymmetry is not invoked), which involve in addition right handed neutrinos…

High Energy Physics - Phenomenology · Physics 2009-11-10 Berthold Stech , Zurab Tavartkiladze

In this letter we try to answer those of the open questions of the Standard model which concern the appearance of families, mass protection mechanism and the Yukawa couplings - by using the approach (proposed by one of us), which suggests a…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Borstnik Bracic , M. Breskvar , D. Lukman , N. S. Mankoc Borstnik

We construct a four-generation MSSM with rank-4 Yukawa matrices from intersecting D6 branes on a T^6/(Z_2 x Z_2) orientifold. The Yukawa matrices obtained provide an example of Flavor Democracy (FD), where the Yukawa couplings are all…

High Energy Physics - Phenomenology · Physics 2011-02-28 A. V. Belitsky , Richard F. Lebed , Van E. Mayes

We present empirical relations that connect the dimensionless ratios of fermion masses for the charged lepton, up-type quark and down-type quark sectors. Explaining these relations from first principles imposes strong constraints on the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Javier Ferrandis

Different approaches to the quark-lepton mass problem are reviewed. The infrared quasifixed point predictions for the top quark mass are discussed for the Standard Model and its minimal supersymmetric extension, with particular reference to…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. D. Froggatt

The observed hierarchy of quark and lepton masses and mixings may be obtained by adding an abelian family symmetry to the Minimal Supersymmetric Model and coupling quarks and leptons to an electroweak singlet scalar field. In a large class…

High Energy Physics - Phenomenology · Physics 2009-10-28 P. Binétruy , S. Lavignac , P. Ramond

In a recent paper, we showed that tree level up-down unification of fermion Yukawa couplings is a natural consequence of a large class of supersymmetric models. They can lead to viable quark masses and mixings for moderately large values of…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. S. Babu , B. Dutta , R. N. Mohapatra

We briefly describe a three-family intersecting D6-brane model in Type IIA theory on the T^6/(Z_2 x Z_2) orientifold with a realistic phenomenology. In this model, the gauge symmetry can be broken down to the Standard Model (SM) gauge…

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

In a supersymmetric model, the presence of a right handed neutrino with a large Yukawa coupling $f_{\nu}$ would affect slepton masses via its contribution to the renormalization group evolution between the grand unification and weak scales.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Howard Baer , Csaba Balazs , J. Kenichi Mizukoshi , Xerxes Tata

In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the exception of neutrino masses. The hierarchies and apparent regularities among the quark and lepton masses are, however, otherwise a mystery.…

High Energy Physics - Phenomenology · Physics 2022-11-07 Sudip Jana , Sophie Klett , Manfred Lindner

We discuss what kinds of combinations of Yukawa interactions can generate the Majorana neutrino mass matrix. We concentrate on the flavor structure of the neutrino mass matrix because it does not depend on details of the models except for…

High Energy Physics - Phenomenology · Physics 2016-01-20 Shinya Kanemura , Hiroaki Sugiyama

By employing D6-branes intersecting at angles in $D = 4$ type IIA strings, we construct {\em four stack string GUT models} (PS-I class), that contain at low energy {\em exactly the three generation Standard model} with no extra matter…

High Energy Physics - Theory · Physics 2016-09-06 Christos Kokorelis

We propose a new mass matrix ansatz: At the grand unified (GU) scale, the standard model (SM) Yukawa coupling matrix elements are integer powers of the square root of the GU gauge coupling constant \varepsilon \equiv…

High Energy Physics - Phenomenology · Physics 2014-11-20 Yong-Chao Zhang , De-Hai Zhang

We suggest the fermion doubling for all quarks and leptons. It is a generalization of the neutrino doubling of the seesaw mechanism. The new quarks and leptons are $SU(2)$ singlets and carry the electromagnetic charges of their lighter…

High Energy Physics - Phenomenology · Physics 2010-11-01 Sanghyeon Chang , Jihn E. Kim

The perturbative leading order open string three-point couplings for the Standard Model with hidden USp(6) on fractional D6-branes on T6/Z6' from arXiv:0806.3039 [hep-th], arXiv:0910.0843 [hep-th] are computed. Physical Yukawa couplings…

High Energy Physics - Theory · Physics 2015-06-03 Gabriele Honecker , Joris Vanhoof

We discuss the unification of the bottom quark and tau lepton Yukawa couplings within the framework of the next-to-minimal supersymmetric standard model. We compare the allowed regions of the $m_t$-$\tan \beta$ plane to those in the minimal…

High Energy Physics - Phenomenology · Physics 2009-10-28 B. C. Allanach , S. F. King

We construct eight-stack intersecting D5-brane models, with an orbifold transverse space, that yield the (non-supersymmetric) standard model up to vector-like leptons. The matter includes right-chiral neutrinos and the models have the…

High Energy Physics - Theory · Physics 2016-09-06 D. Bailin , G. V. Kraniotis , A. Love

We propose a model of fermion masses and mixings based on $SU(5)$ grand unified theory (GUT) and a $D_{4}$ flavor symmetry. This is a highly predictive 4D $SU(5)$ GUT with a flavor symmetry that does not contain a triplet irreducible…

High Energy Physics - Phenomenology · Physics 2021-11-29 M. Miskaoui , M. A. Loualidi

We have considered a general 5D warped model with SM fields propagating in the bulk and computed explicit expressions for oblique and non-oblique electroweak observables as well as for flavor and CP violating effective four-fermion…

High Energy Physics - Phenomenology · Physics 2015-05-30 Joan A. Cabrer , Gero von Gersdorff , Mariano Quiros

We reconsider models of fermion masses and mixings based on a gauge anomalous horizontal U(1) symmetry. In the simplest model with a single flavon field and horizontal charges of the same sign for all Standard Model fields, only very few…

High Energy Physics - Phenomenology · Physics 2014-11-18 P. H. Chankowski , K. Kowalska , S. Lavignac , S. Pokorski