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Related papers: Deformed Intersecting D6-Brane GUTS II

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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

Recently, the complete landscape of three-family supersymmetric Pati-Salam models from intersecting D6-branes on a type IIA $\mathbb{T}^6/(\mathbb{Z}_2\times \mathbb{Z}_2)$ orientifold has been enumerated consisting of 33 independent models…

High Energy Physics - Phenomenology · Physics 2025-02-18 Mudassar Sabir , Adeel Mansha , Tianjun Li , Zhi-Wei Wang

I briefly describe the recent construction of the first specific string D-brane models yielding just the SM massless fermion spectrum. One of the most remarkable facts predicted by these constructions is that the global symmetries of the SM…

High Energy Physics - Phenomenology · Physics 2017-08-23 L. E. Ibanez

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

The minimal embedding of the Standard Model in type I string theory is described. The SU(3) color and SU(2) weak interactions arise from two different collections of branes. The correct prediction of the weak angle is obtained for a string…

High Energy Physics - Theory · Physics 2015-06-26 I. Antoniadis , E. Kiritsis , T. Tomaras

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

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

It is shown that neutrino mixing angles which are consistent with current experimental observations may be naturally obtained in a Pati-Salam model constructed from intersecting D6 branes on a $T^6/(Z_2 \times Z_2)$ orientifold. The Dirac…

High Energy Physics - Phenomenology · Physics 2020-01-08 Van E. Mayes

We consider realizations of GUT models in F-theory. Adopting a bottom up approach, the assumption that the dynamics of the GUT model can in principle decouple from Planck scale physics leads to a surprisingly predictive framework. An…

High Energy Physics - Theory · Physics 2009-11-13 Chris Beasley , Jonathan J. Heckman , Cumrun Vafa

We construct a one-parameter set of intersecting D4-brane models, with six stacks, that yield the (non-supersymmetric) standard model plus extra vector-like matter. Twisted tadpoles and gauge anomalies are cancelled, and the model contains…

High Energy Physics - Theory · Physics 2009-11-07 D. Bailin , G. V. Kraniotis , A. Love

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

Several dimensionful parameters needed for model building can be engineered in a certain class of SU(5) F-theory GUTs by adding extra singlet fields which are localized along pairwise intersections of D7-branes. The values of these…

High Energy Physics - Theory · Physics 2010-02-11 Joseph Marsano , Natalia Saulina , Sakura Schafer-Nameki

The structure of a Standard Model family is derived in a class of brane models with a U(M) x U(N) factor, from two mildly anthropic requirements: a massless photon and a universe that does not turn into a plasma of massless charged…

High Energy Physics - Phenomenology · Physics 2015-06-18 B. Gato-Rivera , A. N. Schellekens

We investigate the construction of four-family ${\cal N}=1$ supersymmetric Pati-Salam models from Type IIA $\mathbb{T}^6/(\mathbb{Z}_2 \times \mathbb{Z}_2)$ orientifold with intersecting D6-branes. Utilizing the deterministic algorithm…

High Energy Physics - Theory · Physics 2022-07-06 Tianjun Li , Rui Sun , Chi Zhang

In hep-th/0703135, they have found the type IIA intersecting brane configuration where there exist three NS5-branes, D4-branes and anti-D4-branes. By analyzing the gravitational interaction for the D4-branes in the background of the…

High Energy Physics - Theory · Physics 2009-04-17 Changhyun Ahn

We construct flipped SU(5) GUT models as Type IIB flux vacua on $\Z_2\times \Z_2$ orientifolds. Turning on supergravity self-dual NSNS and RR three-form fluxes fixes the toroidal complex structure moduli and the dilaton. We give a specific…

High Energy Physics - Theory · Physics 2009-11-11 Ching-Ming Chen , V. E. Mayes , D. V. Nanopoulos

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

We analyze proton decay via dimension six operators in certain GUT-like models derived from Type IIA orientifolds with $D6$-branes. The amplitude is parametrically enhanced by a factor of $\alpha_{GUT}^{-1/3}$ relative to the coresponding…

High Energy Physics - Theory · Physics 2010-04-07 Igor R. Klebanov , Edward Witten

We present new classes of supersymmetric Standard-like models from type IIA $\IT^6/(\IZ_2\times \IZ_2)$ orientifold with intersecting D6-branes. D6-branes can wrap general supersymmetric three-cycles of $\IT^6=\IT^2\times \IT^2\times…

High Energy Physics - Theory · Physics 2009-09-17 Mirjam Cvetic , Ioannis Papadimitriou

We discuss IR limit of four-fermion scattering amplitudes in braneworld models including intersecting-branes and SUSY SU(5) GUT version of it. With certain compactification where instanton effect is negligible, grand unification condition…

High Energy Physics - Phenomenology · Physics 2010-02-03 Piyabut Burikham