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Related papers: Unifying flipped SU(5) in five dimensions

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We construct a four-dimensional SU(5) grand unified theory in which the proton is stable. The Standard Model leptons reside in the 5 and 10 irreps of SU(5), whereas the quarks live in the 40 and 50 irreps. The SU(5) gauge symmetry is broken…

High Energy Physics - Phenomenology · Physics 2017-12-15 Bartosz Fornal , Benjamin Grinstein

We consider five dimensional (5D) supersymmetric SO(10) compactified on the orbifold $S^1/(Z_2\times Z_2')$ such that the SO(10) gauge symmetry is broken on both fixed points (branes), and the residual gauge symmetry is $SU(3)_c\times…

High Energy Physics - Phenomenology · Physics 2010-11-19 Bumseok Kyae , Chin-Aik Lee , Qaisar Shafi

We construct a five dimensional supersymmetric SO(10)$\times$D$_3$ grand unified model with an $S^1/(Z_2 \times Z^\prime_2)$ orbifold as the extra dimension. The orbifold breaks half of the supersymmetry and breaks the SO(10) gauge symmetry…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hyung Do Kim , Stuart Raby , Leslie Schradin

A set of Grand Unified Theories based upon the gauge groups $SU(5)_\L \times SU(5)_\R$, $SO(10)_\L \times SO(10)_\R$ and $SU(4)_\C \times SU(4)_\L \times SU(4)_\R$ is explored. Several novel features distinguish these theories from the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Peter Cho

We briefly review the issues of proton decay and fermion masses and mixings in minimal supersymmetric grand unified theories. We argue that minimal SU(5), although tightly constrained by proton decay data, is still not ruled out. However,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Borut Bajc , Alejandra Melfo , Goran Senjanovic

It is pointed out that a class of flipped SU(5) models based on F-theory naturally explains the gauge coupling unification. It is because the group SU(5) x U(1)_X is embedded in SO(10) and E_8. To prohibit the dimension 4 and 5 proton decay…

High Energy Physics - Theory · Physics 2015-05-27 Kang-Sin Choi , Bumseok Kyae

We have constructed a specific supersymmetric flipped SU(5) GUT model in which bilarge neutrino mixing is incorporated. Because the up-type and down-type quarks in the model are flipped in the representations ten and five with respect to…

High Energy Physics - Phenomenology · Physics 2010-04-05 Chao-Shang Huang , Tianjun Li , Wei Liao

We present the supersymmetric $SU(5)$ models which provide a simple ``all order'' solution to the doublet-triplet splitting problem through the missing doublet mechanism. The crucial role is played by the anomalous $U(1)_A$ gauge symmetry…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zurab Berezhiani , Zurab Tavartkiladze

A unified model is constructed, based on flipped $SU(5)$ in which the proton is absolutely stable. The model requires the existence of new leptons with masses of order the weak scale. The possibility that the unification scale could be…

High Energy Physics - Phenomenology · Physics 2015-06-19 S. M. Barr , X. Calmet

We present an extensive search for a general class of flipped $SU(5)$ models built within the free fermionic formulation of the heterotic string. We describe a set of algorithms which constitute the basis for a computer program capable of…

High Energy Physics - Theory · Physics 2009-10-22 J. Lopez , D. Nanopoulos , K. Yuan

We consider 4-dimensional N=1 supersymmetric SO(10) models inspired by deconstruction of 5-dimensional N=1 supersymmetric orbifold SO(10) models and high dimensional non-supersymmetric SO(10) models with Wilson line gauge symmetry breaking.…

High Energy Physics - Phenomenology · Physics 2009-11-10 Chao-Shang Huang , Jing Jiang , Tianjun Li

A 5D SU(7) family unification model with two spinor representations of SO(14) is presented. The fifth dimension is compactified on $S^1/Z_2\times Z_2'$. The orbifolding is used to obtain 4D SO(10) chiral fermions. The 4D grand unification…

High Energy Physics - Phenomenology · Physics 2009-11-07 Kyuwan Hwang , Jihn E. Kim

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

A realistic grand unified model has never been constructed in the literature due to three major difficulties: the seesaw mechanism without spoiling gauge coupling unification, the doublet-triplet splitting and the proton decay suppression.…

High Energy Physics - Phenomenology · Physics 2017-12-14 Ying-Kang Chen , Da-Xin Zhang

A new supersymmetric grand unified model based on the gauge group $SU(5)\times SU(5)$ is discussed. The model has the feature that the conventional seesaw mechanism for neutrino masses is implemented using the $(15, 1)+(1,\bar{15)}$…

High Energy Physics - Phenomenology · Physics 2009-10-28 R. N. Mohapatra

We explore proton decay in a class of realistic supersymmetric flipped $SU(5)$ models supplemented by a $U(1)_R$ symmetry which plays an essential role in implementing hybrid inflation. Two distinct neutrino mass models, based on inverse…

High Energy Physics - Phenomenology · Physics 2021-02-23 Maria Mehmood , Mansoor Ur Rehman , Qaisar Shafi

We predict the low energy signatures of a Flipped $SU(5) \times U(1)_{\chi}$ effective local model , constructed within the framework of F$-$theory based on $ A_{4} $ symmetry. The Flipped SU(5) model from F Theory in the field of particle…

High Energy Physics - Phenomenology · Physics 2024-04-15 Gayatri Ghosh

We study the supersymmetric spontaneous symmetry breaking of SO(10) into SU(3)xSU(2)xU(1) for the most physically interesting cases of SU(5) or flipped SU(5)xU(1) intermediate symmetries. The first case is more easily realized while the…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. Buccella , C. A. Savoy

We consider explicit unified models based on the flipped ${SU(5)\times U(1)}$ and $SU(6)\times SU(2)$ gauge groups in which gauge mediated proton decay operators are suppressed at leading order due to the special placement of matter fields…

High Energy Physics - Phenomenology · Physics 2014-08-06 A. E. Faraggi , M. Paraskevas , J. Rizos , K. Tamvakis

A product SU(5)xSp(4) grand unified model is proposed with no fundamental Higgs fields transforming under SU(5). Higgs doublets are instead embedded into a four dimensional representation of the Sp(4) gauge group, and hence there is no…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ryuichiro Kitano , Graham D. Kribs