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The LHeC as a Higgs Boson Factory

The LHeC is designed to collide a new 60 GeV energy electron beam, from a 3-pass ERL, with the 7 TeV energy LHC proton beam. At the present target ep luminosity of 1033 cm−2s−1, the LHeC would produce a few 1000 Higgs bosons per year, allowing for precision coupling measurements, especially of the H...

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Detalles Bibliográficos
Autores principales: Zimmermann, F, Bruning, O, Klein, M
Lenguaje:eng
Publicado: 2013
Materias:
Acceso en línea:http://cds.cern.ch/record/1575158
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author Zimmermann, F
Bruning, O
Klein, M
author_facet Zimmermann, F
Bruning, O
Klein, M
author_sort Zimmermann, F
collection CERN
description The LHeC is designed to collide a new 60 GeV energy electron beam, from a 3-pass ERL, with the 7 TeV energy LHC proton beam. At the present target ep luminosity of 1033 cm−2s−1, the LHeC would produce a few 1000 Higgs bosons per year, allowing for precision coupling measurements, especially of the H → b¯b decay in charged current deep inelastic scattering (ep → νHX). With a significant increase of the luminosity, rarer channels become accessible, as the charm decay. Here such an increase, to the level of 1034 cm−2s−1 or even beyond, is considered from a combination of improvements, namely with a smaller proton beam emittance, with a further reduction of the proton IP beta function, an increase of the proton bunch intensity and with doubling the lepton beam current, compared to the canonical values assumed in the CDR.
id cern-1575158
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2013
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spelling cern-15751582019-09-30T06:29:59Zhttp://cds.cern.ch/record/1575158engZimmermann, FBruning, OKlein, MThe LHeC as a Higgs Boson FactoryAccelerators and Storage RingsThe LHeC is designed to collide a new 60 GeV energy electron beam, from a 3-pass ERL, with the 7 TeV energy LHC proton beam. At the present target ep luminosity of 1033 cm−2s−1, the LHeC would produce a few 1000 Higgs bosons per year, allowing for precision coupling measurements, especially of the H → b¯b decay in charged current deep inelastic scattering (ep → νHX). With a significant increase of the luminosity, rarer channels become accessible, as the charm decay. Here such an increase, to the level of 1034 cm−2s−1 or even beyond, is considered from a combination of improvements, namely with a smaller proton beam emittance, with a further reduction of the proton IP beta function, an increase of the proton bunch intensity and with doubling the lepton beam current, compared to the canonical values assumed in the CDR.CERN-ACC-2013-0085oai:cds.cern.ch:15751582013-05-12
spellingShingle Accelerators and Storage Rings
Zimmermann, F
Bruning, O
Klein, M
The LHeC as a Higgs Boson Factory
title The LHeC as a Higgs Boson Factory
title_full The LHeC as a Higgs Boson Factory
title_fullStr The LHeC as a Higgs Boson Factory
title_full_unstemmed The LHeC as a Higgs Boson Factory
title_short The LHeC as a Higgs Boson Factory
title_sort lhec as a higgs boson factory
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/1575158
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