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Related papers: Intersecting Brane Models of Particle Physics and …

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Intersecting D-brane models seem to be one of the most promising avenues to embed the Standard Model physics within the string context. We review here different aspects of these models. Topics include the question of SUSY and quasi-SUSY in…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Cremades , L. E. Ibanez , F. Marchesano

We consider $SU(N)$ $\mathcal{N}=4$ super Yang-Mills with cubic and quadratic soft SUSY breaking potential, such that the global $SU(4)_R$ is broken to $SU(3)$ or further. As shown recently, this set-up supports a rich set of non-trivial…

High Energy Physics - Theory · Physics 2018-04-24 Marcus Sperling , Harold C. Steinacker

We study D-brane inspired models with U(3) x U(2) x U(1)^N gauge symmetry in the context of split supersymmetry. We consider configurations with one, two and three (N=1,2,3) abelian branes and derive all hypercharge embeddings which imply a…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. V. Gioutsos , G. K. Leontaris , A. Psallidas

Recent string constructions with intersecting D6 and D5 brane models succeeded in predicting in the low energy limit a symmetry group and a fermionic spectrum similar to that of the SM. In such constructions additional U(1) fields are a…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. M. Ghilencea

The success of SU(5)-like gauge coupling unification boundary conditions $g_3^2=g_2^2=5/3 g_1^2$ has biased most attempts to embed the SM interactions into a unified structure. After discussing the limitations of the orthodox approach, we…

High Energy Physics - Phenomenology · Physics 2011-03-23 G. Aldazabal , L. E. Ibanez , F. Quevedo

We present what we believe are the first specific string (D-brane) constructions whose low-energy limit yields just a three generation $SU(3)\times SU(2)\times U(1)$ standard model with no extra fermions nor U(1)'s (without any further…

High Energy Physics - Theory · Physics 2015-06-25 L. E. Ibanez , F. Marchesano , R. Rabadan

Following the scanning methods of arXiv:1910.04530, we for the first time systematically construct the $N=1$ supersymmetric $SU(12)_C\times SU(2)_L\times SU(2)_R$ models, $SU(4)_C\times SU(6)_L\times SU(2)_R$ models, and $SU(4)_C\times…

High Energy Physics - Theory · Physics 2023-04-28 Tianjun Li , Adeel Mansha , Rui Sun

We study the structure of Yukawa couplings in intersecting D6-branes wrapping a factorizable 6-torus compact space T^6. Models with MSSM-like spectrum are analyzed and found to fail in predicting the quark mass spectrum because of the way…

High Energy Physics - Phenomenology · Physics 2009-11-10 N. Chamoun , S. Khalil , E. Lashin

In this paper, globally N=1 supersymmetric configurations of intersecting D6-branes on the Z6-orientifold are discussed, involving also fractional branes. It turns out rather miraculously that one is led almost automatically to just ONE…

High Energy Physics - Theory · Physics 2014-11-18 Gabriele Honecker , Tassilo Ott

From the quantum field theory point of view, matter and gauge fields are generally expected to be localised around branes or topological defects occurring in extra dimensions. Here I discuss a simple scenario where, by starting with a five…

High Energy Physics - Theory · Physics 2007-05-23 Gonzalo A. Palma

We study recombinations of D-brane systems intersecting at more than one angle using super Yang-Mills theory. We find the condensation of an off-diagonal tachyon mode relates to the recombination, as was clarified for branes at one angle in…

High Energy Physics - Theory · Physics 2009-11-10 Satoshi Nagaoka

Intersecting stacks of supersymmetric fractional branes on the Z_6' orientifold may be used to construct the supersymmetric Standard Model. If a,b are the stacks that generate the SU(3)_{colour} and SU(2)_L gauge particles, then, in order…

High Energy Physics - Theory · Physics 2019-08-19 David Bailin , Alex Love

We construct four dimensional intersecting D6-brane models that have locally the spectrum of the N=1 Supersymmetric Standard Model. All open {\em visible} string sectors share the same N=1 supersymmetry. As expected in these supersymmetric…

High Energy Physics - Theory · Physics 2007-05-23 Christos Kokorelis

The conventional supersymmetric grand unified theories suffer from two serious problems, the large mass splitting between doublet and triplet Higgs multiplets, and the too long lifetime of the proton. A unification model based on a…

High Energy Physics - Phenomenology · Physics 2009-11-07 Y. Imamura , T. Watari , T. Yanagida

We construct four dimensional three generation non-supersymmetric $SU(3)_c \times SU(2)_L \times U(1)_Y$ intersecting D6-brane models with $\nu_R$\rq{s}. At three stacks we find exactly the MSSM chiral fermion matter spectrum. At 4-,…

High Energy Physics - Theory · Physics 2014-02-19 Christos Kokorelis

By employing D6-branes intersecting at angles in $D = 4$ type IIA strings, we construct {\em four stack string GUT models} (PS-I class), that contain at low energy {\em exactly the three generation Standard model} with no extra matter…

High Energy Physics - Theory · Physics 2016-09-06 Christos Kokorelis

By introducing an extra stack of D6-branes to standard ${\cal N}=1$ supersymmetric Pati-Salam models, we extend the landscape of its complete search. In this construction, the $d$-stack of D6-branes is introduced besides the standard…

High Energy Physics - Theory · Physics 2026-01-09 Haotian Huangfu , Tianjun Li , Qi Sun , Rui Sun

We introduce a simple scenario where, by starting with a five-dimensional SU(3) gauge theory, we end up with several 4-D parallel branes with localized fermions and gauge fields. Similar to the split fermion scenario, the confinement of…

High Energy Physics - Theory · Physics 2009-11-11 Gonzalo A. Palma

We construct an N=1 supersymmetric three-family flipped SU(5) model from type IIA orientifolds on $T^6/(\Z_2\times \Z_2)$ with D6-branes intersecting at general angles. The spectrum contains a complete grand unified and electroweak Higgs…

High Energy Physics - Theory · Physics 2009-11-11 C. -M. Chen , G. V. Kraniotis , V. E. Mayes , D. V. Nanopoulos , J. W. Walker

Recently a class of Type IIA orientifold models was constructed yielding just the fermions of the SM at the intersections of D6-branes wrapping a 6-torus. We generalize that construction to the case of Type IIB compactified on an…

High Energy Physics - Theory · Physics 2016-09-06 D. Cremades , L. E. Ibanez , F. Marchesano
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