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Related papers: Study of Minimal String Unification in $Z_8$ Orbif…

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A distinctive feature of string unification is the possibility of unification by a non-simply-laced group. This occurs most naturally in four dimensional type~II string models where the gauge symmetry is realized by Kac-Moody algebras at…

High Energy Physics - Theory · Physics 2010-11-15 L. Dolan , James T. Liu

Maximally supersymmetric SO(10) and SU(6) unified theories are constructed on the orbifold T^2/(Z_2 x Z'_2), with one length scale R_5 taken much larger than the other, R_6. The effective theory below 1/R_6 is found to be the highly…

High Energy Physics - Phenomenology · Physics 2009-09-29 Lawrence J. Hall , Yasunori Nomura

We construct models of warped unification with a bulk SO(10) gauge symmetry and boundary conditions that preserve the SU(4)_C x SU(2)_L x SU(2)_R Pati-Salam gauge group (422). In the dual 4D description, these models are 422 gauge theories…

High Energy Physics - Phenomenology · Physics 2009-09-29 Yasunori Nomura , David Tucker-Smith

We investigate the low--energy properties of a Z_12 orbifold with continuous Wilson line moduli. They give rise to a (0,2) superstring compactification. Their Kaehler potentials and Yukawa couplings are calculated. We study the discrete…

High Energy Physics - Theory · Physics 2007-05-23 P. Mayr , S. Stieberger

We look for minimal chiral sets of fermions beyond the standard model that are anomaly free and, simultaneously, vectorlike particles with respect to colour SU(3) and electromagnetic U(1). We then study whether the addition of such…

High Energy Physics - Phenomenology · Physics 2015-06-22 Luis M. Cebola , D. Emmanuel-Costa , R. Gonzalez Felipe , C. Simoes

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 2016-09-06 David Bailin , Alex Love

A unification of left-right $\rm{SU}(3)_\rm{L}\times \rm{SU}(3)_\rm{R}$, colour $\rm{SU}(3)_\rm{C}$ and family $\rm{SU}(3)_\rm{F}$ symmetries in a maximal rank-8 subgroup of ${\rm{E}}_8$ is proposed as a landmark for future explorations…

High Energy Physics - Phenomenology · Physics 2019-03-13 José E. Camargo-Molina , António P. Morais , Astrid Ordell , Roman Pasechnik , Jonas Wessén

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

We make a detailed analysis of gauge coupling unification in supersymmetry. When the Standard Model gauge group is embedded in a Grand Unified Theory, new particles often appear below the GUT scale in order to predict the right…

High Energy Physics - Phenomenology · Physics 2008-11-26 Tuhin Roy

A realistic SU(3)_C x SU(3)_W unified theory is constructed with a TeV sized extra dimension compactified on the orbifold S_1/Z_2, leaving only the standard model gauge group SU(3)_C x SU(2)_L x U(1)_Y unbroken in the low energy 4D theory.…

High Energy Physics - Phenomenology · Physics 2009-09-29 Lawrence J. Hall , Yasunori Nomura

We consider the heterotic E8 X E8 string theory, which gives rise to four-dimensional Standard-like Models and allows for their SO(10) embedding. We investigate two different schemes of compactification: the free fermionic formulation and…

High Energy Physics - Theory · Physics 2009-08-24 E. Manno

We describe a class of supersymmetric unified models with the following properties: i) the full breaking of the gauge group is achieved by Higgs fields in the fundamental representation; ii) the correct unification of the strong and…

High Energy Physics - Phenomenology · Physics 2016-09-01 R. Barbieri , G. Dvali , A. Strumia

We consider the renormalisation group flow of gauge couplings within the so-called exceptional supersymmetric standard model (E$_6$SSM) based on the low energy matter content of 27 dimensional representations of the gauge group $E_6$,…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. F. King , S. Moretti , R. Nevzorov

This is a pedagogical review article surveying the various approaches towards understanding gauge coupling unification within string theory. As is well known, one of the major problems confronting string phenomenology has been an apparent…

High Energy Physics - Theory · Physics 2016-09-06 Keith R. Dienes

This paper extends and builds upon the results of an earlier paper, in which we described how to use the tools of geometrical engineering to deform geometrically-engineered grand unified models into ones with lower symmetry. This top-down…

High Energy Physics - Theory · Physics 2008-11-26 Jacob L. Bourjaily

``Anomalous'' U(1) gauge symmetry with Green-Schwarz anomaly cancellation mechanism is discussed in the orbifold construction of four-dimensional heterotic string models. Some conditions are given as criteria to have ``anomalous'' U(1) in…

High Energy Physics - Theory · Physics 2016-09-06 Tatsuo Kobayashi , Hiroaki Nakano

In this short note, we examine the relationship between the string coupling constant, $\gstring{}$, and the grand unified gauge coupling constant, $\alphagut{}$, in a highly successful class of models based on anisotropic orbifold…

High Energy Physics - Theory · Physics 2009-01-10 Ben Dundee , Stuart Raby

We present a minimal model of asymptotic grand unification based on an $SU(5)$ gauge theory in a compact $S^1/(\mathbb{Z}_2 \times \mathbb{Z}'_2)$ orbifold. The gauge couplings run to a unified fixed point in the UV, without supersymmetry.…

High Energy Physics - Theory · Physics 2021-10-20 Giacomo Cacciapaglia , Alan S. Cornell , Corentin Cot , Aldo Deandrea

A Z_2 orbifold compactification of the heterotic string is considered. The resulting 6D GUT groups can be SO(16) or E_7 times SU(2) plus some hidden sector groups. The N=4 supersymmetry is reduced to N=2. In particular, the SO(16) 6D model…

High Energy Physics - Theory · Physics 2009-11-07 Kang-Sin Choi , Jihn E. Kim

We construct a family-unified model on a Z_2xZ_2 orbifold in five dimensions. The model is based on a supersymmetric SU(7) gauge theory. The gauge group is broken by orbifold boundary conditions to a product of grand unified SU(5) and…

High Energy Physics - Phenomenology · Physics 2009-11-10 Zhenyu Han , Witold Skiba
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