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Techniques are presented for computing the cohomology of stable, holomorphic vector bundles over elliptically fibered Calabi-Yau threefolds. These cohomology groups explicitly determine the spectrum of the low energy, four-dimensional…

High Energy Physics - Theory · Physics 2008-11-26 Ron Donagi , Yang-Hui He , Burt A. Ovrut , Rene Reinbacher

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 describe a non-supersymmetric orbifold GUT based on SU(5) symmetry. It is a modification of Kawamura's 5-D orbifold GUT model. The difference lies in the choice of Higgs scalars as we have allowed only 5-plets of SU(5) in the GUT scale.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Biswajoy Brahmachari

We systematically approach the construction of heterotic E_8 X E_8 Calabi-Yau models, based on compact Calabi-Yau three-folds arising from toric geometry and vector bundles on these manifolds. We focus on a simple class of 101 such…

High Energy Physics - Theory · Physics 2010-05-28 Yang-Hui He , Seung-Joo Lee , Andre Lukas

We present a 6D orbifold model on $T^2/\Z2$ which emerges as intermediate step in the compactification of the heterotic string to the supersymmetric standard model in four dimensions. It has $\SU6$ gauge symmetry in the bulk and two pairs…

High Energy Physics - Theory · Physics 2008-11-26 Jonas Schmidt

In this paper we discuss $SU(5)^{3}$ with cyclic symmetry as a possible grand unified theory (GUT). The basic idea of such a tri-unification is that there is a separate $SU(5)$ for each fermion family, with the light Higgs doublet(s)…

High Energy Physics - Phenomenology · Physics 2024-06-27 Mario Fernández Navarro , Stephen F. King , Avelino Vicente

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

We study double-sided actions of $(\mathbb{C}^*)^2$ on $SL(3,\mathbb{C})/U$ and the associated quotients, where $U$ is a maximal unipotent subgroup of $SL(3,\mathbb{C})$. The main results of this paper are a sufficient condition for the…

Algebraic Geometry · Mathematics 2025-11-18 Yoshinori Hashimoto , Hiroaki Ishida , Hisashi Kasuya

We obtain three generation SU(3)_c X SU(2)_L X U(1)_Y string models in all of the exactly solvable (0,2) constructions sampled by fermionization. None of these examples, including those that are symmetric abelian orbifolds, rely on the Z_2…

High Energy Physics - Theory · Physics 2009-10-28 Shyamoli Chaudhuri , George Hockney , Joseph D. Lykken

We study cascade hierarchy in supersymmetric SU(5) grand unified theory. The neutrino Dirac mass matrix of the cascade form can lead to the tri-bimaximal generation mixing at the leading order in the seesaw mechanism while the down quark…

High Energy Physics - Phenomenology · Physics 2010-11-29 Kentaro Kojima , Hideyuki Sawanaka , Ryo Takahashi

The problem of families, "Why are there three families of fermions?", is a long awaited question to be answered within a reasonable framework. We propose anti-SU($N$) groups for the unification of families in grand unification (GUT) groups,…

High Energy Physics - Phenomenology · Physics 2015-06-30 Jihn E. Kim

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

We construct a supersymmetric grand unified model in the framework of a latticized extra dimension. The SU(5) symmetries on the lattice are broken by the vacuum expectation values of the link fields connecting adjacent SU(5) sites, leaving…

High Energy Physics - Phenomenology · Physics 2009-10-09 Hsin-Chia Cheng , Konstantin T. Matchev , Jing Wang

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 study the vacuum structure in 5D SO(10) grand unified theory (GUT) compactified on $S^1/Z_2$ orbifold, where SO(10) is broken into $SU(3)\times SU(2)\times U(1)^2$ through the boundary conditions. Although a lot of people extended to 6D…

High Energy Physics - Phenomenology · Physics 2011-07-19 Naoyuki Haba , Toshifumi Yamashita

Electroweak interactions based on a gauge group $\rm SU(3)_L \times U(1)_X$, coupled to the QCD gauge group $\rm SU(3)_c$, can predict the number of generations to be multiples of three. We first try to unify these models within SU(N)…

High Energy Physics - Phenomenology · Physics 2015-10-07 Pritibhajan Byakti , David Emmanuel-Costa , Arindam Mazumdar , Palash B. Pal

We systematically analyse globally consistent SU(5) GUT models on intersecting D7-branes in genuine Calabi-Yau orientifolds with O3- and O7-planes. Beyond the well-known tadpole and K-theory cancellation conditions there exist a number of…

High Energy Physics - Theory · Physics 2009-09-29 Ralph Blumenhagen , Volker Braun , Thomas W. Grimm , Timo Weigand

The detection of a stochastic background of gravitational waves can reveal details about first-order phase transitions (FOPTs) at a time of $10^{-13}s$ of the early universe. We specifically discuss quiver-type GUTs which avoid both proton…

High Energy Physics - Phenomenology · Physics 2020-11-11 Claudio Corianò , Paul H. Frampton , Alessandro Tatullo

We discuss F-theory SU(5) GUTs in which some or all of the quark and lepton families are assigned to different curves and family symmetry enforces a leading order rank one structure of the Yukawa matrices. We consider two possibilities for…

High Energy Physics - Phenomenology · Physics 2014-11-21 S. F. King , G. K. Leontaris , G. G. Ross

One of the main methods of constructing new spaces with positive or almost positive curvature is the study of biquotients first studied in detail by Eschenburg. We classify orbifold biquotients of the Lie Group $SU(3)$, and construct a new…

Differential Geometry · Mathematics 2015-08-11 Dmytro Yeroshkin