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The \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisited

An optimization of the CERN SPL beam line has been performed guided by the sensitivities to the \theta_{13} mixing angle and to the \delta_{CP} Dirac CP violating phase. A UNO-like 440 ktons water Cerenkov detector located at 130 km from the target in a new foreseen Frejus laboratory has been used a...

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Detalles Bibliográficos
Autores principales: Campagne, Jean Eric, Cazes, Antoine
Lenguaje:eng
Publicado: 2004
Materias:
Acceso en línea:https://dx.doi.org/10.1140/epjc/s2005-02455-x
http://cds.cern.ch/record/805047
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author Campagne, Jean Eric
Cazes, Antoine
author_facet Campagne, Jean Eric
Cazes, Antoine
author_sort Campagne, Jean Eric
collection CERN
description An optimization of the CERN SPL beam line has been performed guided by the sensitivities to the \theta_{13} mixing angle and to the \delta_{CP} Dirac CP violating phase. A UNO-like 440 ktons water Cerenkov detector located at 130 km from the target in a new foreseen Frejus laboratory has been used as a generic detector. Concerning the \delta_{CP} independent \theta_{13} sensitivity, a gain of about 20% may be reached using a 3.5 GeV proton beam with a 40 m long, 2 m radius decay tunnel compared to the up to now considered 2.2 GeV beam energy and 20 m long, 1 m radius decay tunnel. This may motivate new machine developments to upgrade the nominal SPL proton beam energy.
id cern-805047
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2004
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spelling cern-8050472019-09-30T06:29:59Zdoi:10.1140/epjc/s2005-02455-xhttp://cds.cern.ch/record/805047engCampagne, Jean EricCazes, AntoineThe \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisitedParticle Physics - ExperimentAn optimization of the CERN SPL beam line has been performed guided by the sensitivities to the \theta_{13} mixing angle and to the \delta_{CP} Dirac CP violating phase. A UNO-like 440 ktons water Cerenkov detector located at 130 km from the target in a new foreseen Frejus laboratory has been used as a generic detector. Concerning the \delta_{CP} independent \theta_{13} sensitivity, a gain of about 20% may be reached using a 3.5 GeV proton beam with a 40 m long, 2 m radius decay tunnel compared to the up to now considered 2.2 GeV beam energy and 20 m long, 1 m radius decay tunnel. This may motivate new machine developments to upgrade the nominal SPL proton beam energy.hep-ex/0411062LAL-04-102LAL-2004-102oai:cds.cern.ch:8050472004-11-18
spellingShingle Particle Physics - Experiment
Campagne, Jean Eric
Cazes, Antoine
The \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisited
title The \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisited
title_full The \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisited
title_fullStr The \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisited
title_full_unstemmed The \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisited
title_short The \theta_{13} and \delta_{CP} sensitivities of the SPL-Frejus project revisited
title_sort \theta_{13} and \delta_{cp} sensitivities of the spl-frejus project revisited
topic Particle Physics - Experiment
url https://dx.doi.org/10.1140/epjc/s2005-02455-x
http://cds.cern.ch/record/805047
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