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Related papers: Extended SUSY SU(5) predicting type-III seesaw tes…

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We have conceived a supersymmetric Type II seesaw model at TeV scale, which has some additional particles consisting of scalar and fermionic triplet Higgs states, whose masses being around few hundred GeV. In this particular model, we have…

High Energy Physics - Phenomenology · Physics 2015-06-11 R. S. Hundi

Right-handed neutrinos in supersymmetric models can act as the source of lepton flavor violation (LFV). We present experimental implications of lepton flavor-violating processes within a supersymmetric type-I seesaw framework in the…

High Energy Physics - Phenomenology · Physics 2019-10-23 Howard Baer , Vernon Barger , Hasan Serce

A Supersymmetric Grand unified model is constructed based on SO(10)xSO(10) symmetry in which new types of Yukawa matrices couple standard and exotic fermions. Evolution of these couplings from the Grand Unified scale to the electroweak…

High Energy Physics - Phenomenology · Physics 2014-11-17 I. Hinchliffe , N. Kersting

We study the impact of multiple vector-like fermions in SU(5) grand unified theory (GUT). Threshold effects from extra fermions allow the observed gauge couplings to be consistently matched to a single unified gauge coupling, and typically…

High Energy Physics - Phenomenology · Physics 2026-04-10 Akifumi Chitose , Ko Hirooka , Masahiro Ibe , Satoshi Shirai

We discuss the fermion mass problem in SUSY GUTs, including such ideas as texture zeroes, and Georgi-Jarlskog textures. We focus on a specific supersymmetric model based on the gauge group $SU(4)\otimes SU(2)_L \otimes SU(2)_R$. In this…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. C. Allanach , S. F. King

We present a supersymmetric SO(10) grand unified theory (GUT) of flavor based on an $S_4$ family symmetry. It makes use of our recent proposal to use SO(10) with type II seesaw mechanism for neutrino masses combined with a simple ansatz…

High Energy Physics - Phenomenology · Physics 2010-05-28 Bhaskar Dutta , Yukihiro Mimura , R. N. Mohapatra

The masses of vector supermultiplet and of the Higgs supertriplet in standard supersymmetric SU(5) model are calculated. Taking into account uncertainties related with the initial coupling constants and threshold corrections we find that in…

High Energy Physics - Phenomenology · Physics 2009-10-28 N. V. Krasnikov

We present our study of lepton flavour violating decays of a Higgs boson with properties compatible with those of the particle recently discovered at the LHC. We worked in the context of the inverse seesaw model, considering the most…

High Energy Physics - Phenomenology · Physics 2014-06-03 E. Arganda , M. J. Herrero , X. Marcano , C. Weiland

Nonsupersymmetric minimal SU(5) with Higgs representations ${24}_H$ and $5_H$ and standard fermions in ${\bar 5}_F\oplus {10}_F$ is well known for its failure in unification of gauge couplings and lack of predicting neutrino masses. Like…

High Energy Physics - Phenomenology · Physics 2018-08-09 Biswonath Sahoo , Mainak Chakraborty , M. K. Parida

We study the supersymmetric version of the type-II seesaw mechanism assuming minimal supergravity boundary conditions. We calculate branching ratios for lepton flavour violating (LFV) scalar tau decays, potentially observable at the LHC, as…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Hirsch , S. Kaneko , W. Porod

We propose an SU(5) GUT model extended with two additional pairs of $\mathbf{10}$ representation vector-like fermions. The CDF collaboration $W$ boson mass anomaly is explained by using the VEV of a real $\mathrm{SU(2)_L}$ triplet scalar…

High Energy Physics - Phenomenology · Physics 2023-08-09 Yusuke Shimizu , Shonosuke Takeshita

In this work we study an SO(10) GUT model with minimum Higgs representations belonging only to the 210 and 16 dimensional representations of SO(10). We add a singlet fermion S in addition to the usual 16 dimensional representation…

High Energy Physics - Phenomenology · Physics 2009-11-11 Kaushik Bhattacharya , C. R. Das , Bipin R. Desai , G. Rajasekaran , Utpal Sarkar

A simple extension of the minimal renormalizable supersymmetric SO(10) grand unified theory by adding a 120-dimensional Higgs representation is examined. This brings new antisymmetric contributions to the relevant quark and lepton mass sum…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michal Malinsky

The electroweak Higgs doublets are identified as components of a vector multiplet in a higher dimensional supersymmetric field theory. We construct a minimal model in 6D where the electroweak $SU(2) \otimes U(1)$ gauge group is extended to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Lawrence Hall , Yasunori Nomura , David Smith

We suggest a new left-right symmetric grand unified model by extending Pati-Salam group to contain an isospin SU(2) and a flavor SO(3) subgroup, where the superheavy fermions are introduced as a mirror to the low-energy standard model…

High Energy Physics - Phenomenology · Physics 2009-07-22 Wei-Min Yang , Hong-Huan Liu

We study the Minimal Supersymmetric Standard Model (MSSM) constrained by unification assuming mSUGRA SUSY breaking. In particular this means that the three gauge couplings are unified at a {\it per cent} level, third generation yukawa…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Blazek , S. F. King , J. K. Parry

We investigate the LHC discovery potential for electroweak scale heavy neutrino singlets (seesaw I), scalar triplets (seesaw II) and fermion triplets (seesaw III). For seesaw I we consider a heavy Majorana neutrino coupling to the electron…

High Energy Physics - Phenomenology · Physics 2009-11-13 F. del Aguila , J. A. Aguilar-Saavedra

We discuss an $SU(5)$ Grand Unified Theory (GUT) based on the 10d orbifold $(\mathbb{T}^2)^3/(\mathbb{Z}_4\times\mathbb{Z}_2)$ plus three modular $S_4$ groups with moduli at respective fixed points $i,i+2,\omega=e^{2i\pi/3}$. The resulting…

High Energy Physics - Phenomenology · Physics 2024-06-03 Francisco J. de Anda , Stephen F. King

We propose a 6d model with a SUSY $SU(5)$ gauge symmetry. After compactification, it explains the origin of the $S_4$ Family Symmetry with CSD3 vacuum alignment, as well as $SU(5)$ breaking with doublet-triplet splitting. The model…

High Energy Physics - Phenomenology · Physics 2018-07-12 Francisco J. de Anda , Stephen F. King

An $SO(10)$ model where the $10_H$ and $120_H$ representations are used for generating fermion masses is quite predictive, though due to the absence of $SU(2)_{L,R}$ triplet/singlet fields it cannot give rise to neutrino masses through the…

High Energy Physics - Phenomenology · Physics 2015-05-20 Joydeep Chakrabortty , Srubabati Goswami , Amitava Raychaudhuri
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