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Electroweak precision measurements and collider probes of the Standard Model with large extra dimensions

The elementary particles of the Standard Model may live in more than 3+1 dimensions. We study the consequences of large compactified dimensions on scattering and decay observables at high-energy colliders. Our analysis includes global fits to electroweak precision data, indirect tests at high-energy...

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Detalles Bibliográficos
Autores principales: Rizzo, Thomas G., Wells, James D.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.61.016007
http://cds.cern.ch/record/389231
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author Rizzo, Thomas G.
Wells, James D.
author_facet Rizzo, Thomas G.
Wells, James D.
author_sort Rizzo, Thomas G.
collection CERN
description The elementary particles of the Standard Model may live in more than 3+1 dimensions. We study the consequences of large compactified dimensions on scattering and decay observables at high-energy colliders. Our analysis includes global fits to electroweak precision data, indirect tests at high-energy electron-positron colliders (LEP2 and NLC), and direct probes of the Kaluza-Klein resonances at hadron colliders (Tevatron and LHC). The present limits depend sensitively on the Higgs sector, both the mass of the Higgs boson and how many dimensions it feels. If the Higgs boson is trapped on a 3+1 dimensional wall with the fermions, large Higgs masses (up to 500 GeV) and relatively light Kaluza-Klein mass scales (less than 4 TeV) can provide a good fit to precision data. That is, a light Higgs boson is not necessary to fit the electroweak precision data, as it is in the Standard Model. If the Higgs boson propagates in higher dimensions, precision data prefer a light Higgs boson (less than 260 GeV), and a higher compactification scale (greater than 3.8 TeV). Future colliders can probe much larger scales. For example, a 1.5 TeV electron-positron linear collider can indirectly discover Kaluza-Klein excitations up to 31 TeV if 500 fb^-1 integrated luminosity is obtained.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-3892312021-10-08T02:31:13Zdoi:10.1103/PhysRevD.61.016007http://cds.cern.ch/record/389231engRizzo, Thomas G.Wells, James D.Electroweak precision measurements and collider probes of the Standard Model with large extra dimensionsParticle Physics - PhenomenologyThe elementary particles of the Standard Model may live in more than 3+1 dimensions. We study the consequences of large compactified dimensions on scattering and decay observables at high-energy colliders. Our analysis includes global fits to electroweak precision data, indirect tests at high-energy electron-positron colliders (LEP2 and NLC), and direct probes of the Kaluza-Klein resonances at hadron colliders (Tevatron and LHC). The present limits depend sensitively on the Higgs sector, both the mass of the Higgs boson and how many dimensions it feels. If the Higgs boson is trapped on a 3+1 dimensional wall with the fermions, large Higgs masses (up to 500 GeV) and relatively light Kaluza-Klein mass scales (less than 4 TeV) can provide a good fit to precision data. That is, a light Higgs boson is not necessary to fit the electroweak precision data, as it is in the Standard Model. If the Higgs boson propagates in higher dimensions, precision data prefer a light Higgs boson (less than 260 GeV), and a higher compactification scale (greater than 3.8 TeV). Future colliders can probe much larger scales. For example, a 1.5 TeV electron-positron linear collider can indirectly discover Kaluza-Klein excitations up to 31 TeV if 500 fb^-1 integrated luminosity is obtained.The elementary particles of the Standard Model may live in more than 3+1 dimensions. We study the consequences of large compactified dimensions on scattering and decay observables at high-energy colliders. Our analysis includes global fits to electroweak precision data, indirect tests at high-energy electron-positron colliders (LEP2 and NLC), and direct probes of the Kaluza-Klein resonances at hadron colliders (Tevatron and LHC). The present limits depend sensitively on the Higgs sector, both the mass of the Higgs boson and how many dimensions it feels. If the Higgs boson is trapped on a 3+1 dimensional wall with the fermions, large Higgs masses (up to 500 GeV) and relatively light Kaluza-Klein mass scales (less than 4 TeV) can provide a good fit to precision data. That is, a light Higgs boson is not necessary to fit the electroweak precision data, as it is in the Standard Model. If the Higgs boson propagates in higher dimensions, precision data prefer a light Higgs boson (less than 260 GeV), and a higher compactification scale (greater than 3.8 TeV). Future colliders can probe much larger scales. For example, a 1.5 TeV electron-positron linear collider can indirectly discover Kaluza-Klein excitations up to 31 TeV if 500 fb^-1 integrated luminosity is obtained.hep-ph/9906234SLAC-PUB-8119CERN-TH-99-139CERN-TH-99-139SLAC-PUB-8119oai:cds.cern.ch:3892311999-06-04
spellingShingle Particle Physics - Phenomenology
Rizzo, Thomas G.
Wells, James D.
Electroweak precision measurements and collider probes of the Standard Model with large extra dimensions
title Electroweak precision measurements and collider probes of the Standard Model with large extra dimensions
title_full Electroweak precision measurements and collider probes of the Standard Model with large extra dimensions
title_fullStr Electroweak precision measurements and collider probes of the Standard Model with large extra dimensions
title_full_unstemmed Electroweak precision measurements and collider probes of the Standard Model with large extra dimensions
title_short Electroweak precision measurements and collider probes of the Standard Model with large extra dimensions
title_sort electroweak precision measurements and collider probes of the standard model with large extra dimensions
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.61.016007
http://cds.cern.ch/record/389231
work_keys_str_mv AT rizzothomasg electroweakprecisionmeasurementsandcolliderprobesofthestandardmodelwithlargeextradimensions
AT wellsjamesd electroweakprecisionmeasurementsandcolliderprobesofthestandardmodelwithlargeextradimensions