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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

A common way to obtain standard-model-like Lagrangians in string theory is to place D3-branes inside flux compactifications. The bosonic and fermionic masses and couplings of the resulting gauge theory are determined by the ten-dimensional…

High Energy Physics - Theory · Physics 2016-04-13 Iosif Bena , Mariana Graña , Stanislav Kuperstein , Praxitelis Ntokos , Michela Petrini

We construct N=1 supersymmetric fractional branes on the Z_6' orientifold. Intersecting stacks of such branes are needed to build a supersymmetric standard model. If a,b are the stacks that generate the SU(3)_c and SU(2)_L gauge particles,…

High Energy Physics - Theory · Physics 2016-09-06 David Bailin , Alex Love

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 present a consistent string theory model which reproduces the Standard Model, consisting of a D3-brane at a simple orbifold singularity. We study some simple features of the phenomenology of the model. We find that the scale of stringy…

High Energy Physics - Phenomenology · Physics 2009-11-07 David Berenstein , Vishnu Jejjala , Robert G. Leigh

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 2008-12-18 David Bailin , Alex Love

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

Type IIB superstring models with the standard model gauge group on D3-branes and with massless matter associated with open strings joining D3-branes to D3-branes or D3-branes to ${\rm D}7_3$-branes are studied. Models with gauge coupling…

High Energy Physics - Theory · Physics 2009-10-31 D. Bailin , G. V. Kraniotis , A. Love

In this talk, gauge coupling evolution is analyzed in D-brane inspired models with two Higgs doublets and a U(3)xU(2)xU(1)^N gauge symmetry. In particular, we focus on D-brane configurations with two or three abelian factors. We find that…

High Energy Physics - Phenomenology · Physics 2015-06-25 D. V. Gioutsos

We propose a bottom-up approach to the building of particle physics models from string theory. Our building blocks are Type II D-branes which we combine appropriately to reproduce desirable features of a particle theory model: 1) Chirality…

High Energy Physics - Theory · Physics 2009-10-31 G. Aldazabal , L. E. Ibanez , F. Quevedo , A. M. Uranga

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 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 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 construct N=1 supersymmetric fractional branes on the Z_6' orientifold. Intersecting stacks of such branes are needed to build a supersymmetric standard model. If a,b are the stacks that generate the SU(3)_c and SU(2)_L gauge particles,…

High Energy Physics - Theory · Physics 2008-11-26 David Bailin , Alex Love

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

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 describe the main features of new intersecting D4- and D5-brane orbifold 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. There are six-stack…

High Energy Physics - Theory · Physics 2009-11-07 D. Bailin

We investigate left-right symmetric extensions of the standard model based on open strings ending on D-branes, with gauge bosons due to strings attached to stacks of D-branes and chiral matter due to strings stretching between intersecting…

High Energy Physics - Phenomenology · Physics 2017-02-01 Luis A. Anchordoqui , Ignatios Antoniadis , Haim Goldberg , Xing Huang , Dieter Lust , Tomasz R. Taylor

Motivated by D-brane scenarios, we consider a non-supersymmetric model based on the gauge symmetry U(3)_CxU(3)_LxU(3)_R$ which is equivalent to the SU(3)^3 ``trinification'' model supplemented by three U(1)s. Two U(1) combinations are…

High Energy Physics - Phenomenology · Physics 2009-11-11 G. K. Leontaris , J. Rizos

Effective low energy models arising in the context of D-brane configurations with Standard Model (SM) gauge symmetry extended by several gauged abelian factors are discussed. The models are classified according to their hypercharge…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. K. Leontaris , N. D. Tracas , N. D. Vlachos , O. Korakianitis
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