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Related papers: Eliminating the d=5 proton decay operators from SU…

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We realize smooth hybrid inflation in the framework of supersymmetric $SU(5) \times U(1)_{\chi}\subset SO(10)$ model which provides a natural solution to the monopole problem appearing in the spontaneous symmetry breaking of $SU(5)$. The…

High Energy Physics - Phenomenology · Physics 2023-01-18 Waqas Ahmed , Athanasios Karozas , George K. Leontaris , Umer Zubair

The full parameter space of supergravity grand unified theory with $SU(5)$ type $p \rightarrow \bar{\nu} K$ proton decay is analysed using renormalization group induced electroweak symmetry breaking under the restrictions that the universal…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Arnowitt , Pran Nath

Evaluation of nucleon decay modes and branching ratios in a non-minimal supersymmetric SO(10) grand unified theory is presented. The non-minimal GUT considered is the supersymmetrised version of the `realistic' SO(10) model originally…

High Energy Physics - Phenomenology · Physics 2009-10-28 Alick L. Macpherson

Despite the compelling simplicity of minimal supersymmetric unification, the proton does not decay as predicted. A possible explanation is that real unification takes place in a theory which is an electric dual of the MSSM GUT with…

High Energy Physics - Phenomenology · Physics 2010-01-22 Steven Abel , Valentin V. Khoze

In the framework of supersymmetric Grand Unified Theories, the minimal Higgs sector is often extended by introducing multi-dimensional Higgs representations in order to obtain realistic models. However these constructions should remain…

High Energy Physics - Phenomenology · Physics 2009-11-05 Alfredo Aranda , J. Lorenzo Diaz-Cruz , Alma D. Rojas

It is widely believed that minimal supersymmetric SU(5) GUTs have been excluded by the SuperKamiokande bound for the proton decay rate. In the minimal model, however, the theoretical prediction assumes unification of Yukawa couplings,…

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

In a supersymmetric SU(5) grand unified model with a horizontal symmetry SU(1,1), we discuss spontaneous generation of generations to produce three chiral generations of quarks and leptons and one generation of higgses by using one…

High Energy Physics - Phenomenology · Physics 2014-05-07 Naoki Yamatsu

We construct a 5D SUSY SU(6) GUT on an $S^{(1)}/Z_2\tm Z_2'$ orbifold. The first stage of gauge symmetry breaking occurs through compactification and a specific selection of boundary conditions. Additional symmetries play a crucial role for…

High Energy Physics - Phenomenology · Physics 2008-11-26 Filipe Paccetti Correia , Michael G. Schmidt , Zurab Tavartkiladze

The paper addresses the problem of suppressing naturally the unsafe d=4 as well as the color-triplet mediated and/or gravity-linked d=5 proton-decay operators, which generically arise in SUSY-unification. It also attempts to give light…

High Energy Physics - Phenomenology · Physics 2009-10-28 Jogesh C. Pati

The anomalous gauge $U(1)_A$ symmetry which could emerge in the context of the string theories can be very useful ingredient towards builting the complete supersymmetric SO(10) model. We present an example of the $SO(10)\times U(1)_A$ model…

High Energy Physics - Phenomenology · Physics 2009-10-30 Zurab Berezhiani , Zurab Tavartkiladze

We present a comprehensive analysis of a supersymmetric $SO(10)$ Grand Unified Theory, which is broken to the Standard Model via the breaking of two intermediate symmetries. The spontaneous breaking of the first intermediate symmetry,…

High Energy Physics - Phenomenology · Physics 2024-04-01 Bowen Fu , Stephen F. King , Luca Marsili , Silvia Pascoli , Jessica Turner , Ye-Ling Zhou

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

A complete set of Higgs and matter superfields is introduced with well-defined SO(10) properties and U(1) \times Z_2 \times Z_2 family charges from which the Higgs and Yukawa superpotentials are constructed. The Higgs fields solve the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Carl H. Albright , S. M. Barr

$SO(11)$ gauge-Higgs grand unification in the Randall-Sundrum warped space is proposed. Orbifold boundary conditions and one brane scalar field reduce $SO(11)$ to the standard model symmetry, which is further broken to $SU(3)_C \times…

High Energy Physics - Phenomenology · Physics 2015-11-18 Yutaka Hosotani , Naoki Yamatsu

Gauge unification in a five dimensional supersymmetric SO(10) model compactified on an orbifold $S^1/(Z_2 \times Z_2^{\prime})$ is studied. One orbifolding reduces N=2 supersymmetry to N=1, and the other breaks SO(10) to the Pati-Salam…

High Energy Physics - Phenomenology · Physics 2009-11-07 Hyung Do Kim , Stuart Raby

In grand unified theories (GUT) based on SO(10) all fermions of one generation are embedded in a single representation. As a result, the top quark, the bottom quark, and the $\tau$ lepton have a universal Yukawa coupling at the GUT scale.…

High Energy Physics - Phenomenology · Physics 2011-07-19 Ralf Hempfling

We consider proton decay and $g_\mu - 2$ in flipped SU(5) GUT models. We first study scenarios in which the soft supersymmetry-breaking parameters are constrained to be universal at some high scale $M_{in}$ above the standard GUT scale…

High Energy Physics - Phenomenology · Physics 2022-01-05 John Ellis , Jason L. Evans , Natsumi Nagata , Dimitri V. Nanopoulos , Keith A. Olive

The minimal $SO(10)$ grand unified theory, augmented by higher-dimensional operators, is based on the following Higgs representations: adjoint $45_{\rm H}$, spinor $16_{\rm H}$ and complex vector $10_{\rm H}$. It was recently realized that,…

High Energy Physics - Phenomenology · Physics 2024-10-28 Anca Preda , Goran Senjanović , Michael Zantedeschi

Several supersymmetry breaking mechanisms do not produce dimension-3 operators. I show here that this scenario is consistent with present observations and has several significant virtues: i) When there are no dimension-3 SUSY-breaking…

High Energy Physics - Phenomenology · Physics 2007-05-23 Glennys R. Farrar

In a $SU(6)$ gauge theory we found the irreducible representation (175-plet) which does not contain the Higgs doublet. Using this representation we construct two SUSY $SU(6)$ models in which the doublet-triplet splitting occurs naturally,…

High Energy Physics - Phenomenology · Physics 2009-10-28 I. Gogoladze , A. Kobakhidze , Z. Tavartkiladze