Interference effects in the H → γγ + 2 jets channel at LHC

We compute the interference between the resonant process pp → H(→ γγ) + 2 jets and the corresponding continuum background at leading order. For the Higgs signal, we include gluon fusion and vector boson fusion production channels, while for the background we consider all tree-level contributions, in...

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Autores principales: Coradeschi, F., de Florian, D., Fidanza, N., Mazzitelli, J., Narison S.
Formato: JOUR
Acceso en línea:http://hdl.handle.net/20.500.12110/paper_24056014_v258-259_n_p253_Coradeschi
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spelling todo:paper_24056014_v258-259_n_p253_Coradeschi2023-10-03T16:41:22Z Interference effects in the H → γγ + 2 jets channel at LHC Coradeschi, F. de Florian, D. Fidanza, N. Mazzitelli, J. Narison S. We compute the interference between the resonant process pp → H(→ γγ) + 2 jets and the corresponding continuum background at leading order. For the Higgs signal, we include gluon fusion and vector boson fusion production channels, while for the background we consider all tree-level contributions, including pure EW effects (O (αQED)4) and QCD contributions (O (α2QEDα2s). The main effect of the interference is a shift in the peak position of the resonance, which is small in magnitude but strongly dependent on the Higgs width, potentially allowing for a measurement or constraint of the width itself. © 2015 Elsevier B.V. Fil:de Florian, D. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_24056014_v258-259_n_p253_Coradeschi
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
description We compute the interference between the resonant process pp → H(→ γγ) + 2 jets and the corresponding continuum background at leading order. For the Higgs signal, we include gluon fusion and vector boson fusion production channels, while for the background we consider all tree-level contributions, including pure EW effects (O (αQED)4) and QCD contributions (O (α2QEDα2s). The main effect of the interference is a shift in the peak position of the resonance, which is small in magnitude but strongly dependent on the Higgs width, potentially allowing for a measurement or constraint of the width itself. © 2015 Elsevier B.V.
format JOUR
author Coradeschi, F.
de Florian, D.
Fidanza, N.
Mazzitelli, J.
Narison S.
spellingShingle Coradeschi, F.
de Florian, D.
Fidanza, N.
Mazzitelli, J.
Narison S.
Interference effects in the H → γγ + 2 jets channel at LHC
author_facet Coradeschi, F.
de Florian, D.
Fidanza, N.
Mazzitelli, J.
Narison S.
author_sort Coradeschi, F.
title Interference effects in the H → γγ + 2 jets channel at LHC
title_short Interference effects in the H → γγ + 2 jets channel at LHC
title_full Interference effects in the H → γγ + 2 jets channel at LHC
title_fullStr Interference effects in the H → γγ + 2 jets channel at LHC
title_full_unstemmed Interference effects in the H → γγ + 2 jets channel at LHC
title_sort interference effects in the h → γγ + 2 jets channel at lhc
url http://hdl.handle.net/20.500.12110/paper_24056014_v258-259_n_p253_Coradeschi
work_keys_str_mv AT coradeschif interferenceeffectsinthehng2jetschannelatlhc
AT defloriand interferenceeffectsinthehng2jetschannelatlhc
AT fidanzan interferenceeffectsinthehng2jetschannelatlhc
AT mazzitellij interferenceeffectsinthehng2jetschannelatlhc
AT narisons interferenceeffectsinthehng2jetschannelatlhc
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