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Related papers: Deformed Intersecting D6-Brane GUTS and N=1 SUSY

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We propose a minimal embedding of the Standard Model spectrum in a D-brane configuration of type I string theory. The SU(3) color and SU(2) weak interactions arise from two different collections of branes. The model is neither grand unified…

High Energy Physics - Phenomenology · Physics 2009-10-31 I. Antoniadis , E. Kiritsis , T. Tomaras

Non-extremal intersecting p-brane solutions of gravity coupled with several antisymmetric fields and dilatons in various space-time dimensions are constructed. The construction uses the same algebraic method of finding solutions as in the…

High Energy Physics - Theory · Physics 2009-10-30 I. Ya. Aref'eva , M. G. Ivanov , I. V. Volovich

We consider semi-local F-theory GUTs arising from a single E_8 point of local enhancement, leading to simple GUT groups based on E_6, SO(10) and SU(5) with SU(3), SU(4) and SU(5) spectral covers, respectively. Assuming the minimal Z_2…

High Energy Physics - Phenomenology · Physics 2015-05-30 James C. Callaghan , Stephen F. King , George K. Leontaris , Graham G. Ross

Simple supersymmetric SO(10) GUT in five dimensions is proposed, in which the fifth dimension is compactified on the $S^1/(Z_2\times Z_2^\prime)$ orbifold with two inequivalent branes at the orbifold fixed points. In this model, all matter…

High Energy Physics - Phenomenology · Physics 2008-12-30 Takeshi Fukuyama , Nobuchika Okada

We propose a bottom-up approach to the building of particle physics models from string theory. Our building blocks are Type II D-branes which we combine appropriately to reproduce desirable features of a particle theory model: 1) Chirality…

High Energy Physics - Theory · Physics 2009-10-31 G. Aldazabal , L. E. Ibanez , F. Quevedo , A. M. Uranga

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 consider a supersymmetric (SUSY) Grand Unified Theory (GUT) based on the gauge group G_PS=SU(4)_C x SU(2)_L x SU(2)_R, which incorporates non-minimal chaotic inflation, driven by a quartic potential associated with the Higgs fields…

High Energy Physics - Phenomenology · Physics 2011-12-06 C. Pallis , N. Toumbas

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

We perform a detailed study of the grand unified theories $SO(10)$ and $E(6)$ with left-right intermediate gauge symmetries of the form $SU(N)_L\otimes SU(N)_R \otimes \mathcal{G}$. Proton decay lifetime constrains the unification scale to…

High Energy Physics - Phenomenology · Physics 2018-05-16 Joydeep Chakrabortty , Rinku Maji , Subhendra Mohanty , Sunando Kumar Patra , Tripurari Srivastava

We propose a renormalisable model based on $A_4$ family symmetry with an $SU(5)$ grand unified theory (GUT) which leads to the minimal supersymmetric standard model (MSSM) with a two right-handed neutrino seesaw mechanism. Discrete…

High Energy Physics - Phenomenology · Physics 2015-07-01 Fredrik Björkeroth , Francisco J. de Anda , Ivo de Medeiros Varzielas , Stephen F. King

We describe a non-supersymmetric orbifold GUT based on SU(5) symmetry. It is a modification of Kawamura's 5-D orbifold GUT model. The difference lies in the choice of Higgs scalars as we have allowed only 5-plets of SU(5) in the GUT scale.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Biswajoy Brahmachari

In this paper we investigate about several configurations of two intersecting branes at arbitrary angles. We choose the viewpoint of a brane source and a brane probe and use the low-energy dynamics of p-branes. For each p-brane this…

High Energy Physics - Theory · Physics 2007-05-23 Reza Abbaspur

We present a renormalizable non supersymmetric Grand Unified SO(10) model which, at the price of a large fine tuning, is compatible with all compelling phenomenological requirements below the unification scale and thus realizes a minimal…

High Energy Physics - Phenomenology · Physics 2015-06-15 Guido Altarelli , Davide Meloni

We construct a fairy general family of supersymmetric solutions in time- and space-dependent backgrounds in general supergravity theories. One class of the solutions are intersecting brane solutions with factorized form of time- and…

High Energy Physics - Theory · Physics 2010-01-19 Kei-ichi Maeda , Nobuyoshi Ohta , Makoto Tanabe , Ryo Wakebe

We investigate the phase space of parameters in the Pati-Salam model derived in the context of D-branes scenarios, requiring low energy string scale. We find that a non-supersymmetric version complies with a string scale as low as 10 TeV,…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Prikas , N. D. Tracas

We discuss D-branes on a line of conformal field theories connected by an exact marginal deformation. The line contains an SU(2) WZW model and two mutually T-dual SU(2)/U(1) cosets times a free boson. We find the D-branes preserving a U(1)…

High Energy Physics - Theory · Physics 2009-11-07 Stefan Forste

We study supersymmetric intersecting configurations of D-branes with B-field backgrounds. Noncommutative D-brane or M-brane pairs can intersect supersymmetrically over (p-1)-brane, as well as over (p-2)-brane like ordinary branes. d=10 and…

High Energy Physics - Theory · Physics 2009-10-31 Nakwoo Kim

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

We study the introduction of orientifold six-planes in the type IIA brane configurations known as elliptic models. The N=4 SO(n) and $Sp(k)$ theories softly broken to N=2 through a mass for the adjoint hypermultiplet can be realized in this…

High Energy Physics - Theory · Physics 2009-10-09 Angel M. Uranga

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