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Recent work has established a method of constructing non-supersymmetric string models that are stable, with near-vanishing one-loop dilaton tadpoles and cosmological constants. This opens up the tantalizing possibility of realizing stable…

High Energy Physics - Phenomenology · Physics 2018-07-04 Steven Abel , Keith R. Dienes , Eirini Mavroudi

We analyse the cosmological implications of brane-antibrane systems in string-theoretic orbifold and orientifold models. In a class of realistic models, consistency conditions require branes and antibranes to be stuck at different fixed…

High Energy Physics - Theory · Physics 2014-11-18 C. P. Burgess , P. Martineau , F. Quevedo , G. Rajesh , R. -J. Zhang

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

Intersecting Dp-branes often give rise to chiral fermions living on their intersections. We study the construction of four-dimensional chiral gauge theories by considering configurations of type II D(3+n)-branes wrapped on non-trivial…

High Energy Physics - Theory · Physics 2009-10-09 G. Aldazabal , S. Franco , L. E. Ibanez , R. Rabadan , A. M. Uranga

We consider the propagation of Type I open superstrings on orbifolds with four non-compact dimensions and $N=1$ supersymmetry. In this paper, we concentrate on a non-trivial Z_2xZ_2 example. We show that consistency conditions, arising from…

High Energy Physics - Theory · Physics 2009-10-30 M. Berkooz , R. G. Leigh

Intersecting D6-brane models without discrete torsion typically suffer from unstabilized open string moduli, arising from D-brane positions and Wilson lines. These moduli generate additional massless adjoint fields, obstructing the…

High Energy Physics - Theory · Physics 2025-09-05 Adeel Mansha , Mudassar Sabir , Tianjun Li , Luyang Wang

We point out that models where gauge and charged matter fields live on the world volume of D3 branes can provide a weak string coupling description of the gauge coupling unification in the supersymmetric standard model at a scale of order…

High Energy Physics - Phenomenology · Physics 2007-05-23 Erich Poppitz

This article discusses model-building scenarios including anti-D3-/D7-branes, in which supersymmetry is broken spontaneously, despite having no scale at which sparticles appear and standard supersymmetry is restored. If the branes are…

High Energy Physics - Theory · Physics 2022-05-06 Susha Parameswaran , Flavio Tonioni

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

Four stacks of intersecting supersymmetric fractional D6-branes on the Z_6' orientifold have previously been used to construct consistent models having the spectrum of the supersymmetric Standard Model, including a single pair of Higgs…

High Energy Physics - Theory · Physics 2015-05-27 David Bailin , Alex Love

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 systematically analyse globally consistent SU(5) GUT models on intersecting D7-branes in genuine Calabi-Yau orientifolds with O3- and O7-planes. Beyond the well-known tadpole and K-theory cancellation conditions there exist a number of…

High Energy Physics - Theory · Physics 2009-09-29 Ralph Blumenhagen , Volker Braun , Thomas W. Grimm , Timo Weigand

We use the Witten index in the open string sector to determine tadpole charges of orientifold planes and D-branes. As specific examples we consider type I compactifications on Calabi Yau manifolds and noncompact orbifolds. The tadpole…

High Energy Physics - Theory · Physics 2010-11-19 Christian Romelsberger

We show how to construct chiral tachyon-free perturbative orientifold models, where supersymmetry is broken at the string scale on a collection of branes while, to lowest order, the bulk and the other branes are supersymmetric. In higher…

High Energy Physics - Theory · Physics 2009-10-31 I. Antoniadis , E. Dudas , A. Sagnotti

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 a large class of non-supersymmetric AdS-like throat geometries in string theory by taking non-supersymmetric orbifolds of supersymmetric backgrounds. The scale of SUSY breaking is the AdS radius, and the dual field theory has…

High Energy Physics - Theory · Physics 2010-05-27 Shamit Kachru , Dusan Simic , Sandip P. Trivedi

We consider four-dimensional supersymmetric compactifications of the E8 x E8 heterotic string on Calabi-Yau manifolds endowed with vector bundles with structure group SU(N) x U(1) and five-branes. After evaluating the Green-Schwarz…

High Energy Physics - Theory · Physics 2008-11-26 Ralph Blumenhagen , Sebastian Moster , Timo Weigand

We present a six-dimensional T^2/Z_2 orbifold model which arises as an intermediate step in the compactification of the heterotic string to the MSSM. The orbifold contains two pairs of inequivalent fixed points, with unbroken local gauge…

High Energy Physics - Phenomenology · Physics 2007-10-16 C. Lüdeling

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 present a 6D orbifold model on $T^2/\Z2$ which emerges as intermediate step in the compactification of the heterotic string to the supersymmetric standard model in four dimensions. It has $\SU6$ gauge symmetry in the bulk and two pairs…

High Energy Physics - Theory · Physics 2008-11-26 Jonas Schmidt