Search for heavy resonances, and resonant diboson production with the ATLAS detector

Heavy resonances decaying into a pair of fundamental particles such as jj, ℓ+ℓ−, γγ, and ℓV, are among the most common features to search for phenomena beyond the standard model (SM). Electroweak boson pair production, such as WW or ZZ with subsequent decays to ℓVℓ′V′ and ℓℓjj respectively, is a pow...

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Main Author: Tal Hod Noam
Format: Article
Language:English
Published: EDP Sciences 2013-05-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/20134915004
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spelling doaj-c150a149d0214ebc9bbe9fb4ad8b14232021-08-02T11:25:15ZengEDP SciencesEPJ Web of Conferences2100-014X2013-05-01491500410.1051/epjconf/20134915004Search for heavy resonances, and resonant diboson production with the ATLAS detectorTal Hod NoamHeavy resonances decaying into a pair of fundamental particles such as jj, ℓ+ℓ−, γγ, and ℓV, are among the most common features to search for phenomena beyond the standard model (SM). Electroweak boson pair production, such as WW or ZZ with subsequent decays to ℓVℓ′V′ and ℓℓjj respectively, is a powerful test of the spontaneously broken gauge symmetry of the SM and can be also used to search for phenomena beyond the SM. There is a wide spectrum of theoretical models predicting these kinds of resonant signatures. This note covers several searches for these new phenomena conducted within ATLAS in 2011 and 2012 for the LHC 7 and 8 TeV center of mass energies respectively. No significant deviations from the SM have been observed and therefore, limits are set on the characteristic parameters of several new physics models. These benchmark models include new heavy Z′/W′ gauge bosons, chiral excitation of the SM weak gauge bosons, Z*/W* Randal-Sundrum and ADD gravitons, Composite models for quarks, e.g. q* with substructure scale Λ, Quantum black holes, TeV−1 Kaluza-Klein excitation of γ/Z and more. http://dx.doi.org/10.1051/epjconf/20134915004
collection DOAJ
language English
format Article
sources DOAJ
author Tal Hod Noam
spellingShingle Tal Hod Noam
Search for heavy resonances, and resonant diboson production with the ATLAS detector
EPJ Web of Conferences
author_facet Tal Hod Noam
author_sort Tal Hod Noam
title Search for heavy resonances, and resonant diboson production with the ATLAS detector
title_short Search for heavy resonances, and resonant diboson production with the ATLAS detector
title_full Search for heavy resonances, and resonant diboson production with the ATLAS detector
title_fullStr Search for heavy resonances, and resonant diboson production with the ATLAS detector
title_full_unstemmed Search for heavy resonances, and resonant diboson production with the ATLAS detector
title_sort search for heavy resonances, and resonant diboson production with the atlas detector
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2013-05-01
description Heavy resonances decaying into a pair of fundamental particles such as jj, ℓ+ℓ−, γγ, and ℓV, are among the most common features to search for phenomena beyond the standard model (SM). Electroweak boson pair production, such as WW or ZZ with subsequent decays to ℓVℓ′V′ and ℓℓjj respectively, is a powerful test of the spontaneously broken gauge symmetry of the SM and can be also used to search for phenomena beyond the SM. There is a wide spectrum of theoretical models predicting these kinds of resonant signatures. This note covers several searches for these new phenomena conducted within ATLAS in 2011 and 2012 for the LHC 7 and 8 TeV center of mass energies respectively. No significant deviations from the SM have been observed and therefore, limits are set on the characteristic parameters of several new physics models. These benchmark models include new heavy Z′/W′ gauge bosons, chiral excitation of the SM weak gauge bosons, Z*/W* Randal-Sundrum and ADD gravitons, Composite models for quarks, e.g. q* with substructure scale Λ, Quantum black holes, TeV−1 Kaluza-Klein excitation of γ/Z and more.
url http://dx.doi.org/10.1051/epjconf/20134915004
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