U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R

We outline the basic setting of the U ( 3 ) C...

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Main Author: Luis Alfredo Anchordoqui
Format: Article
Language:English
Published: Wiley 2012-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2012/129879
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author Luis Alfredo Anchordoqui
author_facet Luis Alfredo Anchordoqui
author_sort Luis Alfredo Anchordoqui
collection DOAJ
description We outline the basic setting of the U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R gauge theory and review the associated phenomenological aspects related to experimental searches for new physics at hadron colliders. In this construction, there are two massive Z ′-gauge bosons, which can be naturally associated with baryon number B   and   B - L   ( L being lepton number). We discuss the potential signals which may be accessible at the Tevatron and at the Large Hadron Collider (LHC). In particular, we provide the relevant cross sections for the production of Z ′-gauge bosons in the TeV region, leading to predictions that are within reach of the present or the next LHC run. After that we direct attention to embedding the gauge theory into the framework of string theory. We consider extensions of the standard model based on open strings ending on D-branes, with gauge bosons due to strings attached to stacks of D-branes and chiral matter due to strings stretching between intersecting D-branes. Assuming that the fundamental string mass scale is in the TeV range and the theory is weakly coupled, we explore the LHC discovery potential for Regge excitations.
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spelling doaj-art-eeb039a8935c4cac922d39baa36076772025-02-03T01:30:26ZengWileyAdvances in High Energy Physics1687-73571687-73652012-01-01201210.1155/2012/129879129879U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) RLuis Alfredo Anchordoqui0Department of Physics, University of Wisconsin-Milwaukee, P.O. Box 413, Milwaukee, WI 53201, USAWe outline the basic setting of the U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R gauge theory and review the associated phenomenological aspects related to experimental searches for new physics at hadron colliders. In this construction, there are two massive Z ′-gauge bosons, which can be naturally associated with baryon number B   and   B - L   ( L being lepton number). We discuss the potential signals which may be accessible at the Tevatron and at the Large Hadron Collider (LHC). In particular, we provide the relevant cross sections for the production of Z ′-gauge bosons in the TeV region, leading to predictions that are within reach of the present or the next LHC run. After that we direct attention to embedding the gauge theory into the framework of string theory. We consider extensions of the standard model based on open strings ending on D-branes, with gauge bosons due to strings attached to stacks of D-branes and chiral matter due to strings stretching between intersecting D-branes. Assuming that the fundamental string mass scale is in the TeV range and the theory is weakly coupled, we explore the LHC discovery potential for Regge excitations.http://dx.doi.org/10.1155/2012/129879
spellingShingle Luis Alfredo Anchordoqui
U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R
Advances in High Energy Physics
title U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R
title_full U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R
title_fullStr U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R
title_full_unstemmed U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R
title_short U ( 3 ) C × S p ( 1 ) L × U ( 1 ) L × U ( 1 ) R
title_sort u 3 c s p 1 l u 1 l u 1 r
url http://dx.doi.org/10.1155/2012/129879
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