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Related papers: Light vector-like fermions in a minimal SU(5) setu…

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The gauge symmetry of the Standard Model is SU(3)_c x SU(2)_L x U(1)_Y for unknown reasons. One aspect that can be addressed is the low dimensionality of all its subgroups. Why not much larger groups like SU(7), or for that matter, SP(38)…

High Energy Physics - Phenomenology · Physics 2016-12-30 Guillermo Garcia Fernandez , Jesus Guerrero Rojas , Felipe J. Llanes-Estrada

The present work introduces new scalar and fermionic degrees of freedom to the Standard Model. While the scalar sector is augmented by a complex scalar triplet and a doubly charged scalar singlet, the fermionic sector is extended by two…

High Energy Physics - Phenomenology · Physics 2021-11-30 Nabarun Chakrabarty

We extend the left-right symmetric model with an additional non-abelian $SU(2)$ gauge symmetry. The particle content is augmented by one generation of vector-like fermions transforming under the fundamental representation of this new gauge…

High Energy Physics - Phenomenology · Physics 2026-03-10 Yassine Bouzeraib , Mohamed Sadek Zidi

We calculate the oblique electroweak corrections and confront with the experiments in an extension of the Standard Model. The new fields added are a vector-like weak doublet and a singlet fermion. After electroweak symmetry breaking there…

High Energy Physics - Phenomenology · Physics 2008-12-18 G. Cynolter , E. Lendvai

In this paper, we investigate predictions of the SO(10) Grand Unified Theory (GUT), where an extra U(1)$^\prime$ gauge symmetry remains up to the supersymmetry (SUSY) breaking scale. The minimal setup of SO(10) GUT unifies quarks and…

High Energy Physics - Phenomenology · Physics 2017-02-28 Junji Hisano , Yu Muramatsu , Yuji Omura , Yoshihiro Shigekami

It is shown that in realistic SUSY GUT models of quark and lepton masses both the proton decay rate and branching ratios differ in general from those predicted in the minimal $SU(5)$ supersymmetric model. The observation of proton decay,…

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

U(1)-family symmetries have led to successful predictions of the fermion mass spectrum and the mixing angles of the hadronic sector. In the context of the supersymmetric unified theories, they further imply a non-trivial mass structure for…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mario E. Gomez

Apparent regularities in fermion masses and mixings are often associated with physics at a high flavor scale, especially in the context of discrete flavor symmetries. One of the main reasons for that is that the correct vacuum alignment…

High Energy Physics - Phenomenology · Physics 2013-03-14 Martin Holthausen , Manfred Lindner , Michael A. Schmidt

We consider a class of flavored dark matter (DM) theories where dark matter interacts with the Standard Model lepton fields at the renormalizable level. We allow for a general coupling matrix between the dark matter and leptons whose…

High Energy Physics - Phenomenology · Physics 2016-02-17 Mu-Chun Chen , Jinrui Huang , Volodymyr Takhistov

The family symmetry $SU(3)\otimes U(1)$ is proposed to solve flavor problems about fermion masses and flavor mixings. It's breaking is implemented by some flavon fields at the high-energy scale. In addition a discrete group $Z_{2}$ is…

High Energy Physics - Phenomenology · Physics 2015-05-30 Wei-Min Yang , Qi Wang , Jin-Jin Zhong

We study a minimal extension to the Standard Model with an additional real scalar triplet, $\Sigma$, and a single vector-like quark, $T$. This class of models appear naturally in extensions of the Littlest Higgs model that incorporate dark…

High Energy Physics - Phenomenology · Physics 2015-06-22 Estefania Coluccio Leskow , Travis Martin , Alejandro de la Puente

SU(3) gauge theories with increasing number of light fermions are the templates of strongly interacting sectors and studying their low-energy dynamics and spectrum is important, both for understanding the strong dynamics of QCD itself, but…

Pursuing a bottom-up approach to explore which flavor symmetry could serve as an explanation of the observed fermion masses and mixings, we discuss an extension of the standard model (SM) where the flavor structure for both quarks and…

High Energy Physics - Phenomenology · Physics 2011-05-05 C. Hagedorn , M. Lindner , R. N. Mohapatra

We analyze fermion masses and mixing in a general warped extra dimensional model, where all the Standard Model (SM) fields, including the Higgs, are allowed to propagate in the bulk. In this context, a slightly broken flavor symmetry…

High Energy Physics - Phenomenology · Physics 2015-06-10 Mariana Frank , Cherif Hamzaoui , Nima Pourtolami , Manuel Toharia

We consider various constraints on Higgsless models of electroweak symmetry breaking based on a bulk SU(2)_L x SU(2)_R x U(1)_{B-L} gauge group in warped space. First we show that the S parameter which is positive if fermions are localized…

High Energy Physics - Phenomenology · Physics 2009-09-17 Giacomo Cacciapaglia , Csaba Csaki , Christophe Grojean , John Terning

We study extensions of the standard model by one generation of vector-like leptons with non-standard hypercharges, which allow for a sizable modification of the h -> gamma gamma decay rate for new lepton masses in the 300 GeV - 1 TeV range.…

High Energy Physics - Phenomenology · Physics 2022-12-09 Wolfgang Altmannshofer , Martin Bauer , Marcela Carena

Minimal dark matter is an attractive candidate for dark matter because it is stabilized without the need to impose additional symmetries. It is known that the $SU(2)_L$ quintuplet fermion can serve as a minimal dark matter candidate, with…

High Energy Physics - Phenomenology · Physics 2025-03-26 Takashi Toma

There are strong arguments favoring the Flavor Democracy hypothesis (or the Democratic Mass Matrix approach) within the Standard Model framework. However, the large mass of the top quark ($m_t >> m_b, m_\tau$) poses an obstacle to the…

High Energy Physics - Phenomenology · Physics 2026-03-06 Burak Dagli , Saleh Sultansoy , Ismail Toy

The gauge interactions of any supersymmetric extension of the standard model involve new flavor mixing matrices. The assumptions involved in the construction of minimal supersymmetric models, both $SU(3) \times SU(2) \times U(1)$ and grand…

High Energy Physics - Phenomenology · Physics 2009-10-28 Nima Arkani-Hamed , Hsin-Chia Cheng , L. J. Hall

It is appealing to stabilize dark matter by the same discrete symmetry that is used to explain the structure of quark and lepton mass matrices. However, to generate the observed fermion mixing patterns, any flavor symmetry must necessarily…

High Energy Physics - Phenomenology · Physics 2013-05-30 Yuji Kajiyama , Kristjan Kannike , Martti Raidal