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Related papers: Stringy phenomenology with preon models

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A study is made of the implications of heterotic string $T$-duality and extended gauge symmetry for the conjectured equivalence of heterotic and Type I superstrings. While at first sight heterotic string world-sheet dynamics appears to…

High Energy Physics - Theory · Physics 2010-04-07 Joseph Polchinski , Edward Witten

One cannot yet point to any firm string prediction. While many approximate string ground states are known with interesting properties, we do not have any argument that one or another describes what we observe around us, and for reasons…

High Energy Physics - Phenomenology · Physics 2017-08-23 Michael Dine

We find a class of flat supersymmetric brane-antibrane configurations. They follow from ordinary brane-antibrane systems by turning on a specific worldvolume background electric field, which corresponds to dissolved fundamental strings. We…

High Energy Physics - Theory · Physics 2009-11-07 Dongsu Bak , Andreas Karch

We study the symmetry structure of N=8 quantum mechanics, and apply it to the physics of D0-brane probes in type I' string theory. We focus on the theory with a global $Spin(8)$ R symmetry which arises upon dimensional reduction from $2d$…

High Energy Physics - Theory · Physics 2016-09-06 Tom Banks , Nathan Seiberg , Eva Silverstein

Supersymmetric (SUSY) models with heavy sfermions ($m_{\tilde{f}} \sim 10$ TeV) in the first two generations and the third generation sfermion masses below 1 TeV can solve the SUSY flavor and the CP problems as well as satisfy naturalness…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , Chung Kao , Ren-Jie Zhang

These lectures present some topics of string phenomenology and contain two parts. In the first part, I review the possibility of lowering the string scale in the TeV region, that provides a theoretical framework for solving the mass…

High Energy Physics - Theory · Physics 2007-11-08 I. Antoniadis

In discussions of the T-duality between the two heterotic string theories, the duality is actually implemented through the "common" SO(16) x SO(16) subgroup of "SO(32)" and E_8 x E_8. In fact, however, a global investigation shows that no…

High Energy Physics - Theory · Physics 2008-11-26 Brett McInnes

We review the origin of soft supersymmetry-breaking terms in N=1 supergravity models of particle physics. We first consider general formulae for those terms in general models with a hidden sector breaking supersymmetry at an intermediate…

High Energy Physics - Phenomenology · Physics 2016-11-03 A. Brignole , L. E. Ibañez , C. Muñoz

In quantum mechanics, stringnet condensed states - a family of prototypical states exhibiting non-trivial topological order - can be classified via their long-range entanglement properties, in particular topological corrections to the…

Statistical Mechanics · Physics 2014-05-12 M. Hermanns , S. Trebst

This thesis is the discussion of heterotic and type I string phenomenology. The heterotic string model is based on the free--fermionic formalism. This is the first case where non--Abelian VEV's, as opposed to singlet VEV's are required for…

High Energy Physics - Theory · Physics 2007-05-23 D. J. Clements

The Standard Model of particle physics provides very accurate predictions of phenomena occurring at the sub-atomic level, but the reason for the choice of symmetry group and the large number of particles considered elementary, is still…

General Relativity and Quantum Cosmology · Physics 2015-06-29 Daniel Cartin

The general form of soft supersymmetry breaking terms at one loop for effective supergravity models based on the weakly-coupled heterotic string are presented, with special emphasis on those terms arising from the superconformal anomaly.…

High Energy Physics - Phenomenology · Physics 2017-08-23 Brent D. Nelson

String theory compactifications come with numerous $U(1)$ factors, implying the presence of many hidden photons in the low-energy EFT. One may call this the ``string photoverse''. We argue that, generically, these hidden photons are…

High Energy Physics - Theory · Physics 2025-12-01 Thibaut Coudarchet , Arthur Hebecker , Joerg Jaeckel , Jonathan Steiner

Talk given at the 26th Workshop: ``From Superstrings to Supergravity" Erice - Sicily, 5-12 December 1992: In this talk we discuss string consistency requirements on four dimensional string models, namely the cancellation of target space…

High Energy Physics - Theory · Physics 2007-05-23 Dieter Luest

The Pentagon Model is an explicit supersymmetric extension of the Standard Model, which involves a new strongly-interacting SU(5) gauge theory at TeV-scale energies. We discuss embeddings of the Pentagon Model into string theory,…

High Energy Physics - Theory · Physics 2010-05-04 Sean Echols

We explore the possibility of embedding the Pati-Salam model in the context of Type I brane models. We study a generic model with U(4)_C x U(2)_L x U(2)_R gauge symmetry and matter fields compatible with a Type I brane configuration.…

High Energy Physics - Phenomenology · Physics 2014-11-17 G. K. Leontaris , J. Rizos

The generic supersymmetric version of the Standard Model would have the minimal list of superfields incorporating the Standard Model particles, and a Lagrangian dictated by the Standard Model gauge symmetries. To be phenomenologically…

High Energy Physics - Phenomenology · Physics 2014-11-17 Otto C. W. Kong

We provide a study of the phenomenology of orbifold compactifications of the heterotic string within the context of supergravity effective theories. Our investigation focuses on those models where the soft Lagrangian is dominated by loop…

High Energy Physics - Phenomenology · Physics 2017-08-23 Y. Mambrini

We consider heterotic string theories in nine and eight dimensions. We identify the disconnected part of the spacetime gauge group by studying the outer automorphism of the charge lattices. The absence of the global symmetry indicates the…

High Energy Physics - Theory · Physics 2025-10-08 Yuta Hamada , Arata Ishige

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