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Related papers: Standard Model at Intersecting D5-branes: Lowering…

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We investigate intersecting D6-branes on an orientifold of type IIA theory in the orbifold background T^6/(Z_4 x Z_2) with the emphasis on finding chiral spectra. RR tadpole cancellation conditions and the scalar potential at disc level are…

High Energy Physics - Theory · Physics 2010-04-05 Gabriele Honecker

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 study supersymmetric intersecting D6-branes wrapping 3-cycles in the Type IIA T^6/Z_4 orientifold background. As a new feature, the 3-cycles in this orbifold space arise both from the untwisted and the Z_2 twisted sectors. We present an…

High Energy Physics - Theory · Physics 2009-11-07 Ralph Blumenhagen , Lars Goerlich , Tassilo Ott

For recently constructed classes of D6-brane models, yielding the Standard Model fermion spectrum and gauge symmetry, we compute lower bounds on the masses of new U(1) fields that such models predict in addition to the hypercharge $U(1)_Y$.…

High Energy Physics - Phenomenology · Physics 2011-03-23 D. M. Ghilencea

We study the Fayet-Iliopoulos (FI) D-terms on D-branes in type II Calabi-Yau backgrounds. We provide a simple worldsheet proof of the fact that, at tree level, these terms only couple to scalars in closed string hypermultiplets. At the…

High Energy Physics - Theory · Physics 2008-11-26 Albion Lawrence , John McGreevy

Starting from a peculiar orientifold projection proposed long ago by Angelantonj and Cardella, we elaborate on a novel perturbative scenario that involves only D-branes, together with the two types of orientifold planes ${\rm O}_{\pm}$ and…

High Energy Physics - Theory · Physics 2021-07-28 Thibaut Coudarchet , Emilian Dudas , Hervé Partouche

We develop tools for analyzing the space of intersecting brane models. We apply these tools to a particular T^6/Z_2^2 orientifold which has been used for model building. We prove that there are a finite number of intersecting brane models…

High Energy Physics - Theory · Physics 2010-10-27 Michael R. Douglas , Washington Taylor

We construct new supersymmetric SU(5) Grand Unified Models based on Z4 x Z2 orientifolds with intersecting D6-branes. Unlike constructions based on Z2 x Z2 orientifolds, the orbifold images of the three-cycles wrapped by D6-branes…

High Energy Physics - Theory · Physics 2008-11-26 Mirjam Cvetic , Paul Langacker

Discrete gauge symmetries in global intersecting D-brane models constrain the exact form of the perturbative as well as non-perturbative superpotential. We derive the complete set of conditions on the existence of discrete Zn gauge…

High Energy Physics - Theory · Physics 2013-11-06 Gabriele Honecker , Wieland Staessens

We present brane constructions in Type IIA string theory for N=1 supersymmetric SO and Sp gauge theories with tensor representations using an orientifold 6-plane. One limit of these set-ups corresponds to N=2 theories previously constructed…

High Energy Physics - Theory · Physics 2009-09-17 Csaba Csaki , Martin Schmaltz , Witold Skiba , John Terning

Generalizing three-family chiral fermion conditions to $I_{ac}=-(3+h)$ and $I_{ac'}=h$, with positive integer $h$, we extend the landscape of three-family ${\cal N}=1$ supersymmetric Pati-Salam models in a broader region. Differing from the…

High Energy Physics - Theory · Physics 2025-12-19 Tianjun Li , Qi Sun , Rui Sun , Lina Wu

We study Type I string theory compactified on a T^6/Z_3 orientifold. The low-energy dynamics is most conveniently analyzed in terms of D3-branes. We show that a sector of the theory, which corresponds to placing an odd number of D3-branes…

High Energy Physics - Theory · Physics 2014-11-18 Joseph Lykken , Erich Poppitz , Sandip P. Trivedi

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 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

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 construct the type IIA nonsupersymmetric meta-stable brane configurations corresponding to the various N=1 supersymmetric gauge theories. The D6-branes are both displaced and rotated where these deformations are described as the mass…

High Energy Physics - Theory · Physics 2009-11-05 Changhyun Ahn

We show that previous proposals to accommodate the MSSM with string theory N=0 non-supersymmetric compactifications coming from intersecting D6-branes may be made fully consistent with the cancellation of RR tadpoles. In this respect we…

High Energy Physics - Theory · Physics 2007-05-23 Emmanuel Floratos , Christos Kokorelis

Is perturbative stability intimately tied with the existence of spacetime fermions in string theory in more than two dimensions? Type 0'B string theory in ten-dimensional flat space is a rare example of a non-tachyonic, non-supersymmetric…

High Energy Physics - Theory · Physics 2009-04-17 Dan Israel , Vasilis Niarchos

Using a ``Superstrings with Torsion'' type description, we study a class of IIB orientifolds in which spacefilling O5 planes and D5 branes wrap the T^2 fiber in a warped modification of the product of 4D Minkowski space and a T^2 fibration.…

High Energy Physics - Theory · Physics 2009-11-10 Michael B. Schulz

A while ago, examples of N=1 vacua in D=6 were constructed as orientifolds of Type IIB string theory compactified on the K3 surface. Among the interesting features of those models was the presence of D5-branes behaving like small…

High Energy Physics - Theory · Physics 2009-10-30 Eric G. Gimon , Clifford V. Johnson