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Related papers: Low Energy Consequences of Five Dimensional SO(10)

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We present in this talk a model based on SO(10) x SU(2)_{F} having symmetric mass textures with 5 zeros constructed by us recently. The symmetric mass textures arising from the left-right symmetry breaking chain of SO(10) give rise to good…

High Energy Physics - Phenomenology · Physics 2015-06-25 Mu-Chun Chen , K. T. Mahanthappa

It is shown that embedding of flipped SU(5) in a five-dimensional SO(10) enables exact unification of the gauge coupling constants. The demand for the unification uniquely determines both the compactification scale and the cutoff scale.…

High Energy Physics - Phenomenology · Physics 2010-11-19 I. Dorsner

Generic SO(10) GUT models suffer from the problem that Planck scale induced non-renormalizable proton decay operators require extreme suppression of their couplings to be compatible with present experimental upper limits. One way to resolve…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. N. Mohapatra , A. T. Azatov

A good fit of the fermion masses and mixings has been found in the minimal renormalizable supersymmetric SO(10). This solution needs a strongly split supersymmetry breaking scenario with gauginos and higgsinos around 100 TeV, sfermions…

High Energy Physics - Phenomenology · Physics 2009-01-06 Borut Bajc , Ilja Dorsner , Miha Nemevsek

We review the main constraints on the parameter space of the minimal renormalizable supersymmetric SU(5) grand unified theory. They consist of the Higgs mass, proton decay, electroweak symmetry breaking and fermion masses. Superpartner…

High Energy Physics - Phenomenology · Physics 2015-06-17 Borut Bajc , Stephane Lavignac , Timon Mede

We discuss inflationary cosmology in a five dimensional SO(10) model compactified on $S^1/(Z_2\times Z_2')$, which yields $SU(3)_c\times SU(2)_L\times U(1)_Y\times U(1)_X$ below the compactification scale. The gauge symmetry $SU(5)\times…

High Energy Physics - Phenomenology · Physics 2014-11-17 Bumseok Kyae , Qaisar Shafi

We investigate a 5D SU(6) grand gauge-Higgs unification model compactified on an orbifold S^1/Z_2. Ordinary quarks and leptons, together with right-handed neutrinos, are just accommodated into a minimal set of representations of the gauge…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. S. Lim , Nobuhito Maru

We consider a supersymmetric model motivated by a SO(10) grand unified theory: the gauge sector near the supersymmetry scale consists of SU(3)_c x SU(2)_L x U(1)_R x U(1)_{B-L}. We embed this model in minimal gauge mediation and incorporate…

High Energy Physics - Phenomenology · Physics 2013-08-06 Manuel E. Krauss , Werner Porod , Florian Staub

It is noted that a set of facts points to the relevance in four dimensions of conventional supersymmetric unification based on minimally a string-unified G(224)-symmetry, or maximally SO(10). These include: (i) the observed family-…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jogesh C. Pati

We review minimal realistic grand unified models based on $SU(5)$ and $SO(10)$ gauge groups. The models with small Higgs representations and higher dimensional operators - under the assumption of no cancellations in proton decay amplitudes…

High Energy Physics - Phenomenology · Physics 2023-07-27 Goran Senjanović , Michael Zantedeschi

We present a minimal renormalizable non-supersymmetric SO(10) grand unified model with a symmetry breaking sector consisting of Higgs fields in the 54_H + 126_H + 10_H representations. This model admits a single intermediate scale…

High Energy Physics - Phenomenology · Physics 2015-10-21 K. S. Babu , S. Khan

We discuss some phenomenological aspects of gauged supersymmetric $\gs$--models on homogeneous coset-spaces $\ESO$ and $SO(10)/U(5)$ which are some of the most interesting for phenomenology. We investigate in detail the vacuum…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. S. Nyawelo

We study the breaking of a supersymmetric SO(10) GUT in 6 dimensions by orbifold compactification. In 4 dimensions we obtain a N=1 supersymmetric theory with the standard model gauge group enlarged by an additional U(1) symmetry. The…

High Energy Physics - Phenomenology · Physics 2014-11-17 T. Asaka , W. Buchmüller , L. Covi

In the context of supersymmetric $SO(10)$ grand unified models, it is shown that the gauge symmetry breaking as well as a natural doublet--triplet splitting can be achieved with a minimal Higgs system consisting of a single adjoint and a…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr

We embed the minimal left-right model SU(2)_L*SU(2)_R* U(1)_{B-L} into an SU(4)_W gauge group, and break the unified group via five-dimensional S^1/(Z_2*Z_2) orbifolding. Leptons are fitted into SU(4)_W multiplets and located on a symmetry…

High Energy Physics - Phenomenology · Physics 2009-09-07 Csaba Balazs , Tianjun Li , Fei Wang , Jin Min Yang

We consider supersymmetric SO(10) grand unification where the unified gauge group can break to the Standard Model gauge group through different chains. The breaking of SO(10) necessarily involves the reduction of the rank, and consequent…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Ananthanarayan , P. N. Pandita

We study Gauge-Higgs Unification in five dimensions on the lattice by means of the mean-field expansion. We formulate it for the case of an SU(2) pure gauge theory and orbifold boundary conditions along the extra dimension, which explicitly…

High Energy Physics - Lattice · Physics 2015-06-05 Nikos Irges , Francesco Knechtli , Kyoko Yoneyama

We provide a unified description of fermion masses and mixing angles in the framework of a supersymmetric grand unified SO(10) model with anarchic Yukawa couplings of order unity. The space-time is five dimensional and the extra flat…

High Energy Physics - Phenomenology · Physics 2015-07-03 Ferruccio Feruglio , Ketan M. Patel , Denise Vicino

We investigate the presence of discrete gauge symmetries in Grand Unification models based in $SO(10)$ and $E_6$. These models include {\it flipped} and {\it unflipped} $SU(5)$, $SU(4)\!\times\! SU(2)_L\!\times\! SU(2)_R$,…

High Energy Physics - Phenomenology · Physics 2009-10-22 M. De Montigny , M. Masip

We embed the flipped SU(5) models into the SO(10) models. After the SO(10) gauge symmetry is broken down to the flipped SU(5) \times U(1)_X gauge symmetry, we can split the five/one-plets and ten-plets in the spinor \mathbf{16} and…

High Energy Physics - Phenomenology · Physics 2010-02-03 Chao-Shang Huang , Tianjun Li , Chun Liu , Jonathan P. Shock , Feng Wu , Yue-Liang Wu