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Related papers: Non-supersymmetric Orientifolds of Gepner Models

200 papers

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 discuss the construction of six- and four-dimensional Type IIB orientifolds with vanishing untwisted RR tadpoles, but generically non-zero twisted RR tadpoles. Tadpole cancellation requires the introduction of D-brane systems with zero…

High Energy Physics - Theory · Physics 2009-10-31 R. Rabadan , A. M. Uranga

We check the list of supersymmetric standard model orientifold spectra of Dijkstra, Huiszoon and Schellekens for the presence of global anomalies, using probe branes. Absence of global anomalies is found to impose strong constraints, but in…

High Energy Physics - Theory · Physics 2008-11-26 B. Gato-Rivera , A. N. Schellekens

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

We construct intersecting D5-brane orbifold models that yield the (non-supersymmetric) standard model up to vector-like matter and charged-singlet scalars. The models are constrained by the requirement that twisted tadpoles cancel, and that…

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

We consider certain four dimensional supersymmetric and non-supersymmetric asymmetric orbifolds with vanishing cosmological constant up to two loops and gauge the world sheet parity transformation. This leads to new string vacua, in which…

High Energy Physics - Theory · Physics 2009-10-31 Ralph Blumenhagen , Lars Goerlich

This thesis contains an introductory chapter on orbifolds. The following chapter explains the foundations of orientifolds. Chapters 4-7 present own research. In chapter 4 we quantize open strings with linear boundary conditions, as they…

High Energy Physics - Theory · Physics 2009-09-29 Lars Goerlich

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

In the presence of internal magnetic fields, a D9 brane can acquire a D5 (or anti-D5) R-R charge, and can therefore contribute to the corresponding tadpole. In the resulting vacua, supersymmetry is generically broken and tachyonic…

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

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…

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

In a recent work, Tachikawa and Zhang proved the existence of a discrete topological term in the unique non-supersymmetric heterotic string with no tachyons in ten dimensions. This theory features NS5-branes, whose chiral degrees of freedom…

High Energy Physics - Theory · Physics 2025-07-17 Ivano Basile , Vittorio Larotonda

We investigate orientifolds of type II string theory on K3 and Calabi-Yau 3-folds with intersecting D-branes wrapping special Lagrangian cycles. We determine quite generically the chiral massless spectrum in terms of topological invariants…

High Energy Physics - Theory · Physics 2009-11-07 Ralph Blumenhagen , Volker Braun , Boris Kors , Dieter Lust

We consider closed string tachyons localized at the fixed points of noncompact nonsupersymmetric orbifolds. We argue that tachyon condensation drives these orbifolds to flat space or supersymmetric ALE spaces. The decay proceeds via an…

High Energy Physics - Theory · Physics 2009-11-07 A. Adams , J. Polchinski , E. Silverstein

A system of k Neveu-Schwarz (NS) 5-branes of type II string theory with one transverse direction compactified on a circle admits various unstable D-brane systems, - some with geometric instability arising out of being placed at a point of…

High Energy Physics - Theory · Physics 2009-11-13 Ashoke Sen

We describe a new class of supersymmetric orientifolds which combine the world-sheet parity transformation with a complex conjugation in the compact directions. As an example, we investigate in detail the orientifold of the Z_3 toroidal…

High Energy Physics - Theory · Physics 2009-09-25 Ralph Blumenhagen , Lars Goerlich , Boris Kors

We review physical motivations and possible realizations of string vacua with large internal volume and/or low string scale and discuss the issue of supersymmetry breaking. In particular, we describe the key features of Scherk-Schwarz…

High Energy Physics - Theory · Physics 2014-11-18 I. Antoniadis , A. Sagnotti

We determine all D-branes in the non-tachyonic 0'B orientifold, examine their world-volume anomalies and study orbifold compactifications. We find that the spectrum of the D-branes contains chiral fermions in the symmetric, antisymmetric…

High Energy Physics - Theory · Physics 2010-11-19 E. Dudas , J. Mourad

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 study the type II string vacua with chiral space-time SUSY constructed as asymmetric orbifolds of torus and $ K3 $ compactifications. Despite the fact that all the D-branes are non-BPS in any chiral SUSY vacua, we show that the relevant…

High Energy Physics - Theory · Physics 2017-09-13 Yuji Satoh , Yuji Sugawara , Takahiro Uetoko

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