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Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeV

At CLIC and the ILC beam–beam forces lead to the emission of beamstrahlung photons and a reduction of the effective center-of-mass energy. This degradation is controlled by the choice of the horizontal beam size. A reduction of this parameter would increase the luminosity but also the beamstrahlung....

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Detalles Bibliográficos
Autores principales: Andrianala, F., Raboanary, R., Roloff, P., Schulte, D.
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2016.10.046
http://cds.cern.ch/record/2270287
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author Andrianala, F.
Raboanary, R.
Roloff, P.
Schulte, D.
author_facet Andrianala, F.
Raboanary, R.
Roloff, P.
Schulte, D.
author_sort Andrianala, F.
collection CERN
description At CLIC and the ILC beam–beam forces lead to the emission of beamstrahlung photons and a reduction of the effective center-of-mass energy. This degradation is controlled by the choice of the horizontal beam size. A reduction of this parameter would increase the luminosity but also the beamstrahlung. In this paper the optimum choice for the horizontal beam size is investigated for one of the most important physics processes. The Higgsstrahlung process $e^+ e^− \to HZ$ is identified in a model-independent manner by observing the Z boson and determining the mass against which it is recoiling. The physics analysis for this process is performed for constant running times, assuming different beam size and taking into account the resulting levels of integrated luminosity and the associated luminosity spectra.
id oai-inspirehep.net-1501816
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2017
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spelling oai-inspirehep.net-15018162019-09-30T06:29:59Zdoi:10.1016/j.nima.2016.10.046http://cds.cern.ch/record/2270287engAndrianala, F.Raboanary, R.Roloff, P.Schulte, D.Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeVAccelerators and Storage RingsAt CLIC and the ILC beam–beam forces lead to the emission of beamstrahlung photons and a reduction of the effective center-of-mass energy. This degradation is controlled by the choice of the horizontal beam size. A reduction of this parameter would increase the luminosity but also the beamstrahlung. In this paper the optimum choice for the horizontal beam size is investigated for one of the most important physics processes. The Higgsstrahlung process $e^+ e^− \to HZ$ is identified in a model-independent manner by observing the Z boson and determining the mass against which it is recoiling. The physics analysis for this process is performed for constant running times, assuming different beam size and taking into account the resulting levels of integrated luminosity and the associated luminosity spectra.oai:inspirehep.net:15018162017
spellingShingle Accelerators and Storage Rings
Andrianala, F.
Raboanary, R.
Roloff, P.
Schulte, D.
Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeV
title Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeV
title_full Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeV
title_fullStr Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeV
title_full_unstemmed Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeV
title_short Beam parameter optimization at CLIC using the process $e^+e^− \to HZ \to Hq \bar q$ at 380 GeV
title_sort beam parameter optimization at clic using the process $e^+e^− \to hz \to hq \bar q$ at 380 gev
topic Accelerators and Storage Rings
url https://dx.doi.org/10.1016/j.nima.2016.10.046
http://cds.cern.ch/record/2270287
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