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Related papers: An Orbifold Compactification with Three Families f…

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We construct new Standard-like models on Type II orientifolds. In Type IIA theory on $\mathbf{T^6/(\Z_2\times \Z_2)}$ orientifold with intersecting D6-branes, we first construct a three-family trinification model where the $U(3)_C\times…

High Energy Physics - Theory · Physics 2008-11-26 Ching-Ming Chen , Tianjun Li , Dimitri V. Nanopoulos

We present a six-dimensional T^2/Z_2 orbifold model which arises as an intermediate step in the compactification of the heterotic string to the MSSM. The orbifold contains two pairs of inequivalent fixed points, with unbroken local gauge…

High Energy Physics - Phenomenology · Physics 2007-10-16 C. Lüdeling

We study the possibility of family unification on the basis of SO(2N) gauge theory on the five-dimensional space-time, $M^4\times S^1/Z_2$. Several SO(10), $SU(4) \times SU(2)_L \times SU(2)_R$ or SU(5) multiplets come from a single bulk…

High Energy Physics - Phenomenology · Physics 2010-04-22 Yoshiharu Kawamura , Takashi Miura

We consider the possibility of grand unification of the $\mathrm{ SU(3)_c \otimes SU(3)_L \otimes U(1)_X}$ model in an SU(6) gauge unification group. Two possibilities arise. Unlike other conventional grand unified theories, in SU(6) one…

High Energy Physics - Phenomenology · Physics 2016-10-07 Frank F. Deppisch , Chandan Hati , Sudhanwa Patra , Utpal Sarkar , Josè W. F. Valle

A unification of left-right $\rm{SU}(3)_\rm{L}\times \rm{SU}(3)_\rm{R}$, colour $\rm{SU}(3)_\rm{C}$ and family $\rm{SU}(3)_\rm{F}$ symmetries in a maximal rank-8 subgroup of ${\rm{E}}_8$ is proposed as a landmark for future explorations…

High Energy Physics - Phenomenology · Physics 2019-03-13 José E. Camargo-Molina , António P. Morais , Astrid Ordell , Roman Pasechnik , Jonas Wessén

We build a supersymmetric version with $SU(3)_C\otimes SU(2)_L\otimes U(1)_{Y^\prime}\otimes U(1)_{B-L}$ gauge symmetry, where $Y^\prime$ is a new charge and $B$ and $L$ are the usual baryonic and leptonic numbers. The model has three…

High Energy Physics - Phenomenology · Physics 2017-06-14 J. C. Montero , V. Pleitez , M. C. Rodriguez , B. L. Sánchez-Vega

In the context of the local gauge group $SU(3)_c\otimes SU(3)_L\otimes U(1)_X$, we look for possible four family models, where all the particles carry ordinary electric charges. Thirteen different anomaly-free fermion structures emerge, out…

High Energy Physics - Phenomenology · Physics 2014-11-21 Richard H. Benavides , William A. Ponce , Yithsbey Giraldo

Based on the Z_{12-I} orbifold compactification of the heterotic string theory, we construct a flipped-SU(5) model with three families of the standard model matter and ingredients for dynamical supersymmetry breaking. The doublet-triplet…

High Energy Physics - Phenomenology · Physics 2009-12-31 Ji-Haeng Huh , Jihn E. Kim , Bumseok Kyae

Many four-dimensional supersymmetric compactifications of F-theory contain gauge groups that cannot be spontaneously broken through geometric deformations. These "non-Higgsable clusters" include realizations of $SU(3)$, $SU(2)$, and $SU(3)…

High Energy Physics - Theory · Physics 2015-06-23 Antonella Grassi , James Halverson , Julius Shaneson , Washington Taylor

Phenomenological evidence suggests the existence of non-trivial background fields in the QCD vacuum. On the other hand SU(3) gauge theory possessses three different classes of both non-generic and non-trivial strata that may be used as…

High Energy Physics - Theory · Physics 2007-05-23 R. Vilela Mendes

We modify a recently proposed heterotic model hep-th/0703210, giving three net-generations of standard model fermions, to get rid of an additional U(1) factor in the gauge group. The method employs a stable SU(5) bundle on a Calabi-Yau…

High Energy Physics - Theory · Physics 2008-11-26 Bjorn Andreas , Gottfried Curio

We extend the unitary groups beyond the ${\rm SU}(5)$ and ${\rm SU}(6)$ to look for possible grand unified theories that give rise to three-generational Standard Model fermions without the simple repetition. By demanding asymptotic free…

High Energy Physics - Phenomenology · Physics 2022-02-03 Ning Chen

A three-family non-supersymmetric model with U(3)^3 gauge symmetry is analyzed in the context of intersecting D-branes. This is equivalent to the `trinification' model extended by three U(1) factors which survive as global symmetries in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. K. Leontaris

We classify N=1 orbifolds on the E_6 root lattice and investigate explicit model constructions on the Z_3xZ_3 orbifold in heterotic string theory. Interestingly some of the twisted sectors from the Z_3xZ_3 orbifold on the E_6 root lattice…

High Energy Physics - Theory · Physics 2008-11-26 Kei-Jiro Takahashi

Pisano and Pleitez have introduced an interesting $\mbox{SU}(3)_C \otimes \mbox{SU}(3)_L \otimes \mbox{U}(1)_N$ gauge model which has the property that gauge anomaly cancellation requires the number of generations to be a multiple of 3. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 Robert Foot , Hoang Ngoc Long , Tuan A. Tran

The data from collider experiments and cosmic observatories indicates the existence of three light matter generations. In some classes of string compactifications the number of generations is related to a topological quantity, the Euler…

High Energy Physics - Theory · Physics 2010-04-05 Ron Donagi , Alon E. Faraggi

We describe a family of genus one fibered Calabi-Yau threefolds with fundamental group ${\mathbb Z}/2$. On each Calabi-Yau $Z$ in the family we exhibit a positive dimensional family of Mumford stable bundles whose symmetry group is the…

Algebraic Geometry · Mathematics 2008-11-26 Ron Donagi , Burt Ovrut , Tony Pantev , Dan Waldram

We realize a supersymmetric trinification model with three families of $({\bf 27}_{\rm tri}+{\bf 27}_{\rm tri} +\bar{\bf 27}_{\rm tri})$ by the $Z_3$ orbifold compactification with two Wilson lines. It is possible to break the trinification…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jihn E. Kim

We study the construction of the minimal supersymmetric standard model from the $Z_8$ orbifold models. We use a target-space duality anomaly cancellation and a unification of gauge couplings as constraints. It is shown that some models…

High Energy Physics - Theory · Physics 2009-10-22 H. Kawabe , T. Kobayashi , N. Ohtsubo

We propose a realistic flipped SU(5) model derived from a five-dimensional orbifold SO(10) model. The Standard Model (SM) fermion masses and mixings are explained by combining the traditional Froggatt-Nielsen mechanism with the…

High Energy Physics - Phenomenology · Physics 2010-03-02 Csaba Balazs , Zhaofeng Kang , Tianjun Li , Fei Wang , Jin Min Yang
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