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Related papers: Deformed Intersecting D6-Brane GUTS I

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

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

We analyze the construction of non-supersymmetric three generation six-stack Pati-Salam (PS) $SU(4)_C \times SU(2)_L \times SU(2)_R$ GUT classes of models, by localizing D6-branes intersecting at angles in four dimensional orientifolded…

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

By employing D6-branes intersecting at angles in $D = 4$ type I strings, we construct the first examples of three generation string GUT models (PS-A class), that contain at low energy exactly the standard model spectrum with no extra matter…

High Energy Physics - Theory · Physics 2009-11-07 Christos Kokorelis

I discuss two types of non-supersymmetric string model constructions that give at low energy exactly the Standard model (SM) with no additional matter/and or gauge group factors. The construction is based on D6 branes intersecting at angles…

High Energy Physics - Theory · Physics 2017-08-23 Christos Kokorelis

We provide a general overview of the current state of the art in three generation model building proposals - using intersecting D-brane toroidal compactifications of IIA string theories - which have, only, the SM at low energy. In this…

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

We discuss the first string theory examples of three generation non-supersymmetric SU(5) and {\em flipped} SU(5) GUTS, which break to the Standard model at low energy, without extra matter and/or gauge group factors. Our GUT examples are…

High Energy Physics - Theory · Physics 2016-09-06 Minos Axenides , Emmanuel Floratos , Christos Kokorelis

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

We construct new D6-brane model vacua (non-supersymmetric) that have at low energy exactly the standard model spectrum (with right handed neutrinos). The minimal version of these models requires five stacks of branes. and the construction…

High Energy Physics - Theory · Physics 2009-11-07 Christos Kokorelis

We construct a new set of intersecting D4-brane models that yield the (non-supersymmetric) standard model up to vector-like matter and, in some cases, extra U(1) factors in the gauge group. The models are constrained by the requirement that…

High Energy Physics - Theory · Physics 2010-04-05 D. Bailin , G. V. Kraniotis , A. Love

We provide a general overview of the current state of the art in four dimensional three generation model building proposals - using intersecting D-brane toroidal compactifications [without fluxes] of IIA, IIB string theories - which have…

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

We discuss the construction of four dimensional non-supersymmetric models obtained from configurations of D6-branes intersecting at angles. We present the first examples of string GUT models which break exactly to the Standard Model (SM) at…

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

We construct six stack D6-brane vacua (non-supersymmetric) that have at low energy exactly the standard model (with right handed neutrinos). The construction is based on D6-branes intersecting at angles in $D = 4$ type toroidal orientifolds…

High Energy Physics - Theory · Physics 2014-11-18 Christos Kokorelis

We discuss the appearance of non-supersymmetric D6-brane GUT model constructions. We focus on the construction of the first examples of flipped SU(5) and SU(5) GUTS which have only the SM at low energy. These constructions are based on 4D…

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

All the possible three-family ${\cal N}=1$ supersymmetric Pati-Salam models constructed with intersecting D6-branes from Type IIA orientifolds on $T^6/(\mathbb{Z}_2\times \mathbb{Z}_2)$ are recently presented in arXiv: 2112.09632. Taking…

High Energy Physics - Theory · Physics 2022-08-17 Weikun He , Tianjun Li , Rui Sun , Lina Wu

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

We provide a systematic construction of three-family N=1 supersymmetric Pati-Salam models from Type IIA orientifolds on $\IT^6/(\IZ_2\times \IZ_2)$ with intersecting D6-branes. All the gauge symmetry factors $SU(4)_C\times SU(2)_L \times…

High Energy Physics - Theory · Physics 2009-09-17 Mirjam Cvetic , Tianjun Li , Tao Liu

We construct three quasi-supersymmetric $G^3$ GUT models with $S_3$ symmetry and gauge coupling unification from intersecting D6-branes on Type IIA orientifolds. The Standard Model fermions and Higgs doublets can be embedded into the…

High Energy Physics - Theory · Physics 2015-06-26 Tianjun Li , Tao Liu

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

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

We briefly describe a three-family intersecting D6-brane model in Type IIA theory on the T^6/(Z_2 x Z_2) orientifold with a realistic phenomenology. In this model, the gauge symmetry can be broken down to the Standard Model (SM) gauge…

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