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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

A recent D-brane model designed to accommodate a phenomenologically acceptable fourth generation of chiral fermions was noted to produce an unexpected additional unbroken nonanomalous U(1) gauge group at the string scale. We show that the…

High Energy Physics - Phenomenology · Physics 2011-10-27 Richard F. Lebed , Van E. Mayes

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 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 study a class of type I string models with supersymmetry broken on the world-volume of some D-branes and vanishing tree-level potential. Despite the non-supersymmetric spectrum, supersymmetry is non-linearly realized on these D-branes,…

High Energy Physics - Theory · Physics 2015-06-26 I. Antoniadis , K. Benakli , A. Laugier

We perform a systematic study of the Standard Model embedding in a D-brane configuration of type I string theory at the TeV scale. We end up with an attractive model and we study several phenomenological questions, such as gauge coupling…

High Energy Physics - Theory · Physics 2008-11-26 I. Antoniadis , E. Kiritsis , J. Rizos , T. N. Tomaras

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

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

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

Generic D-brane string models of particle physics predict the existence of extra U(1) gauge symmetries beyond hypercharge. These symmetries are not of the E_6 class but rather include the gauging of Baryon and Lepton numbers as well as…

High Energy Physics - Phenomenology · Physics 2011-09-29 D. M. Ghilencea , L. E. Ibanez , N. Irges , F. Quevedo

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 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 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 propose two supersymmetric Standard Models (SMs) with decaying and stable dark matter (DM) particles. To explain the SM fermion masses and mixings and have a heavy decay DM particle S, we consider the Froggatt-Nielsen mechanism by…

High Energy Physics - Phenomenology · Physics 2014-11-20 Xin Gao , Zhaofeng Kang , Tianjun Li

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 construct the first three family N=1 supersymmetric string model with Standard Model gauge group SU(3)_C x SU(2)_L x U(1)_Y from an orientifold of type IIA theory on T^6/(Z_2 x Z_2) and D6-branes intersecting at angles. In addition to…

High Energy Physics - Theory · Physics 2008-11-26 Mirjam Cvetic , Gary Shiu , Angel M. Uranga

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

We propose a non-universal U(1)'_F symmetry combined with the Minimal Supersymmetric Standard Model. All anomaly cancellation conditions are satisfied without exotic fields other than three right-handed neutrinos. Because our model allows…

High Energy Physics - Phenomenology · Physics 2014-11-21 Mu-Chun Chen , Jinrui Huang

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

We propose a renormalizable theory based on the $SU(3)_C\times SU(3)_L\times U(1)_X$ gauge symmetry, supplemented by the spontaneously broken $U(1)_{L_g}$ global lepton number symmetry and the $S_3 \times Z_2 $ discrete group, which…

High Energy Physics - Phenomenology · Physics 2021-03-08 A. E. Cárcamo Hernández , Yocelyne Hidalgo Velásquez , Sergey Kovalenko , H. N. Long , Nicolás A. Pérez-Julve , V. V. Vien
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