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Related papers: Flavored Orbifold GUT - an SO(10) x S4 model

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We construct a compactification of the heterotic string on an orbifold T^6/Z_6 leading to the standard model spectrum plus vector--like matter. The standard model gauge group is obtained as an intersection of three SO(10) subgroups of E_8.…

High Energy Physics - Phenomenology · Physics 2010-11-19 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Michael Ratz

We construct supersymmetric (SUSY) grand unification (GUT) models in the six dimensional space-time where the GUT symmetry is broken down to the standard-model gauge group by a simple orbifolding T^2/Z_4 or T^2/Z_6 and a pair of massless…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. Watari , T. Yanagida

Asymmetric tri-bi-maximal mixing is a recently proposed, grand unified theory (GUT) based, flavor mixing scheme. In it, the charged lepton mixing is fixed by the GUT connection to down-type quarks and a $\mathcal{T}_{13}$ flavor symmetry,…

High Energy Physics - Phenomenology · Physics 2020-11-24 Salvador Centelles Chuliá , Andreas Trautner

We suggest simple models which produce the suitable fermion mass hierarchies and flavor mixing angles based on the supersymmetric SO(10) grand unified theory in 6 dimensions compactified on a T^2/Z_2 orbifold. The gauge and Higgs fields…

High Energy Physics - Phenomenology · Physics 2009-11-07 N. Haba , T. Kondo , Y. Shimizu

We describe a supersymmetric Grand Unified Theory based on the gauge group $\SU(5)^3$, or $\SO(10)^3$, invariant under the interchange of any~SU(5), or~SO(10), with each family multiplet transforming non trivially under one different…

High Energy Physics - Phenomenology · Physics 2009-10-09 Riccardo Barbieri , Gia Dvali , Alessandro Strumia

We construct a flavor model in an anti-SU(5) GUT with a tetrahedral symmetry $A_4$. We choose a basis where $Q_{text{em}}=-\frac13$ quarks and charged leptons are already mass eigenstates. This choice is possible from the $A_4$ symmetry.…

High Energy Physics - Phenomenology · Physics 2020-03-25 Paul H. Frampton , Jihn E. Kim , Se-Jin Kim , Soonkeon Nam

A simple supersymmetric SO(10) GUT in five dimensions is considered. The fifth dimension is compactified on the $S^1/(Z_2\times Z_2^\prime)$ orbifold possessing two inequivalent fixed points. In our setup, all matter and Higgs multiplets…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takeshi Fukuyama , Nobuchika Okada

We study proton decay in a supersymmetric {\sf SO(10)} gauge theory in six dimensions compactified on an orbifold. The dimension-5 proton decay operators are forbidden by R-symmetry, whereas the dimension-6 operators are enhanced due to the…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Buchmuller , L. Covi , D. Emmanuel-Costa , S. Wiesenfeldt

The horizontal symmetry $U(3)_H$ can greatly help in solving the flavor problems in the supersymmetric grand unification. We consider the $SU(5)\times U(3)_H$ model and show that it leads to the remarkable relations between the fermion mass…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zurab Berezhiani

We review SO(10) grand unified theories (GUTs) in four and five dimensions (4D and 5D). The renormalizable minimal SO(10) SUSY GUT is the central theme of this review. It is very predictive and makes it possible to construct all mass…

High Energy Physics - Phenomenology · Physics 2015-06-12 Takeshi Fukuyama

We investigate gauge coupling unification in higher dimensional GUT models with split supersymmetry. We focus on 5d and 6d orbifold GUTs, which permit a simple solution to several problems of 4D GUTs as well as control over GUT scale…

High Energy Physics - Phenomenology · Physics 2009-11-10 Philip C. Schuster

Beyond Standard Model physics frequently connects flavor symmetry with a discrete group. If the discrete symmetry arises spontaneously from a gauge theory, one can maintain compatibility with quantum gravity and avoid anomalies. We provide…

High Energy Physics - Phenomenology · Physics 2018-12-18 Bradley L. Rachlin , Thomas W. Kephart

In the standard model matter fields form complete representations of a grand unified group whereas Higgs fields belong to incomplete `split' multiplets. This remarkable fact is naturally explained by `local grand unification' in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Michael Ratz

We consider 5d SU(5) GUT models based on the orbifold $S^1/(Z_2 \times Z_2')$, and study the different possibilities of placing the SU(5) matter multiplets in three possible locations, namely, the two branes at the two orbifold fixed points…

High Energy Physics - Phenomenology · Physics 2009-11-11 Gautam Bhattacharyya , Amitava Raychaudhuri

We propose a supersymmetric SU(5) orbifold GUT in 5 dimensions in which supersymmetry breaking at the boundaries give rise to split supersymmetry spectrum. The extra dimension is compactified on a $S^1/Z_2 \times Z_2^\prime$ orbifold having…

High Energy Physics - Phenomenology · Physics 2014-11-18 Utpal Sarkar

We study a finite SU(5) grand unified model based on the non-Abelian discrete symmetry A_4. This model leads to the democratic structure of the mass matrices for the quarks and leptons. In the soft supersymmetry breaking sector, the scalar…

High Energy Physics - Phenomenology · Physics 2009-11-07 K. S. Babu , Tatsuo Kobayashi , Jisuke Kubo

I review a recent work on gauged flavor with left-right symmetry, where all masses and all Yukawa couplings owe their origin to spontaneous flavor symmetry breaking. This is suggested as a precursor to a full understanding of flavor of…

High Energy Physics - Phenomenology · Physics 2015-06-05 Rabindra N. Mohapatra

Recent discovery of neutrino large mixings implies the large mixings in the diagonalizing matrices of $\bf\bar 5$ fields in $SU(5)$ grand unified theory (GUT), while the diagonalizing matrices of $\bf 10$ fields of $SU(5)$ are expected to…

High Energy Physics - Phenomenology · Physics 2017-02-23 Nobuhiro Maekawa , Yu Muramatsu

After we study the 6-dimensional ${\cal N} = (1, 1)$ supersymmetry breaking and $R$ symmetry breaking on $M^4\times T^2/Z_n$, we construct two ${\cal N} = (1, 1)$ supersymmetric $E_6$ models on $M^4\times T^2/Z_3$ where $E_6$ is broken down…

High Energy Physics - Phenomenology · Physics 2014-11-17 Tianjun Li

We show how gauge coupling unification is successfully implemented through non-supersymmetric grand unified theory, $SO(10)\times G_f (~G_f=S_4, SO(3)_f, SU(3)_f)$, using low-scale flavor symmetric model of the type $SU(2)_L\times U(1)_Y$ $…

High Energy Physics - Phenomenology · Physics 2011-05-20 Mina K. Parida , Pradip K. Sahu , Kalpana Bora
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