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Related papers: Proton Decay and Sub-Structure

200 papers

We make a first systematic study of non-universal TeV scale neutral gauge bosons $Z'$ arising naturally from a class of F-theory inspired models broken via $SU(5)$ by flux. The phenomenological models we consider may originate from…

High Energy Physics - Phenomenology · Physics 2018-05-23 Miguel Crispim Romao , Stephen F. King , George K. Leontaris

Non-uniform structures of the nucleon matter are expected at subnuclear densities and above the nuclear density: they are called nuclear pastas and kaon pastas, respectively. We numerically study these phases by means of the density…

Giving up the solutions to the fine-tuning problems, we propose the non-supersymmetric flipped $SU(5)\times U(1)_X$ model based on the minimal particle content principle, which can be constructed from the four-dimensional $SO(10)$ models,…

High Energy Physics - Phenomenology · Physics 2018-01-23 Heng-Yu Chen , Ilia Gogoladze , Shan Hu , Tianjun Li , Lina Wu

A review of the current status of nucleon stability in SUSY unified models is given. The review includes analysis of nucleon stability in the minimal SU(5) supergravity model, and in extensions of the minimal model such as SO(10) models,…

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

We calculate the proton decay rate due to five dimensional SU(5) gauge bosons in the Randall-Sundrum scenario with two branes (Planck brane and TeV brane). We consider matter in the usual 10 and \bar 5 SU(5) representations localized on a…

High Energy Physics - Phenomenology · Physics 2014-11-17 Shrihari Gopalakrishna

We consider the constraints from proton decay and $b$-$\tau$ unification in the minimal supersymmetric SU(5) grand unified theory with a `visible' dynamical supersymmetry breaking sector. We show how the presence of vector-like messenger…

High Energy Physics - Phenomenology · Physics 2009-09-29 Christopher D. Carone , Hitoshi Murayama

In a model of supersymmetric SU(5) Grand Unification with a spatial dimension described by the orbifold $S^1/(Z_2 \times Z_2')$, proton decay is naturally suppressed at all orders. This is achieved by a suitable implementation of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gautam Bhattacharyya , K. Sridhar

We discuss the common features between the Standard Model taxonomy of particles, based on electric charge, strangeness and isospin, and the taxonomy emerging from the key structural elements of the rotating neutrino model, which describes…

General Physics · Physics 2016-07-01 Constantinos G. Vayenas , Athanasios S. Fokas , Dimitrios P. Grigoriou

The electroweak (EW) symmetry breaking in the simplest supersymmetric (SUSY) extensions of the standard model (SM), i.e. minimal and next-to-minimal supersymmetric standard models (MSSM and NMSSM), is considered. The spectrum of the Higgs…

High Energy Physics - Phenomenology · Physics 2011-05-13 R. Nevzorov

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

The present paper is based upon ideas and results obtained in an earlier paper by the author devoted to a new formulation of quantum electrodynamics. The equations derived in that paper depict the structure and properties of the electron as…

General Physics · Physics 2017-05-08 V. A. Golovko

It is shown that non-renormalizable gravitational interactions in the Higgs sector of supersymmetric grand unified theories (GUT's) can produce the breaking of the unifying gauge group $G$ at the GUT scale $M_{\rm GUT} \sim 10^{16}$~GeV.…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Urano , D. Ring , R. Arnowitt

In supersymmetry, there are gauge invariant dimension 5 proton decay operators which must be suppressed by a mass scale much larger than the Planck mass. It is natural to expect that this suppression should be explained by a mechanism that…

High Energy Physics - Phenomenology · Physics 2009-11-07 Mitsuru Kakizaki , Masahiro Yamaguchi

We consider semi-local F-theory GUTs arising from a single E_8 point of local enhancement, leading to simple GUT groups based on E_6, SO(10) and SU(5) with SU(3), SU(4) and SU(5) spectral covers, respectively. Assuming the minimal Z_2…

High Energy Physics - Phenomenology · Physics 2015-05-30 James C. Callaghan , Stephen F. King , George K. Leontaris , Graham G. Ross

The conventional signature for grand unified theories (GUT) is the proton decay. Recently, some models in extra dimensions or with specific discrete symmetries, which aim at solving the doublet-triplet problem, allow the color-triplet in…

High Energy Physics - Phenomenology · Physics 2009-11-07 Kingman Cheung , Gi-Chol Cho

In this short note we describe the symmetry responsible for absolute, nonperturbative proton stability in the Standard Model. The SM with $N_c$ colors and ${N_g}$ generations has an exact, anomaly-free, generation-independent, global…

High Energy Physics - Phenomenology · Physics 2022-07-13 Seth Koren

The "proton size puzzle" and the "muon anomalous moment problem" are incomplete descriptions of significant discrepancies of Standard Model calculations with experiments. What is particularly new is that the experiments and theory confront…

High Energy Physics - Phenomenology · Physics 2016-06-21 John Craig Martens , John P. Ralston

The consequences of the charge symmetry breaking effects of the mass difference between the up and down quarks and electromagnetic effects for searches for strangeness form factors in parity violating electron scattering from the proton are…

Nuclear Theory · Physics 2008-11-26 Gerald A. Miller

A model is proposed in which quarks, leptons and perhaps gauge bosons are composites of magnetically charged rishons T(q=1/3) and V(q=0) with magnetic charges g=(1,2,-3)g0. Structural formulas of composite particles and their interactions…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. Heuson

We discuss how realistic supersymmetric models can be constructed by employing an anomalous ${\cal U}(1)$ flavor symmetry which also mediates supersymmetry breaking. A judicious choice of ${\cal U}(1)$ charges enables the first two squark…

High Energy Physics - Phenomenology · Physics 2011-05-12 Qaisar Shafi , Zurab Tavartkiladze