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Design of the Superconducting Section of the SPL LINAC at CERN

In order to set up a powerful proton source for a future Neutrino Factory, increasing at the same time the flux of protons available for new and existing facilities, CERN is studying a 2.2 GeV superconducting H- linac for 4 MW beam power, called SPL. The superconducting part of this linac covers the...

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Detalles Bibliográficos
Autores principales: Gerigk, F, Vretenar, R D, Ryne, M
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:http://cds.cern.ch/record/509986
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author Gerigk, F
Vretenar, R D
Ryne, M
author_facet Gerigk, F
Vretenar, R D
Ryne, M
author_sort Gerigk, F
collection CERN
description In order to set up a powerful proton source for a future Neutrino Factory, increasing at the same time the flux of protons available for new and existing facilities, CERN is studying a 2.2 GeV superconducting H- linac for 4 MW beam power, called SPL. The superconducting part of this linac covers the energy range from 120 MeV to 2.2 GeV. Three sections made of 352 MHz cavities with nominal ß of 0.52, 0.7 and 0.8 bring the beam energy up to 1 GeV. From this energy, superconducting cavities from LEP, or ß =0.8 cavities, can be used to reach the final energy of 2.2 GeV. This paper covers the optimisation for the superconducting part, the beam dynamics design principles, the matching between sections, and the results of multiparticle simulations with up to 50 million particles. To demonstrate the stability of the design matched and mismatched input beams are used.
id cern-509986
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
record_format invenio
spelling cern-5099862023-06-23T09:23:02Zhttp://cds.cern.ch/record/509986engGerigk, FVretenar, R DRyne, MDesign of the Superconducting Section of the SPL LINAC at CERNAccelerators and Storage RingsIn order to set up a powerful proton source for a future Neutrino Factory, increasing at the same time the flux of protons available for new and existing facilities, CERN is studying a 2.2 GeV superconducting H- linac for 4 MW beam power, called SPL. The superconducting part of this linac covers the energy range from 120 MeV to 2.2 GeV. Three sections made of 352 MHz cavities with nominal ß of 0.52, 0.7 and 0.8 bring the beam energy up to 1 GeV. From this energy, superconducting cavities from LEP, or ß =0.8 cavities, can be used to reach the final energy of 2.2 GeV. This paper covers the optimisation for the superconducting part, the beam dynamics design principles, the matching between sections, and the results of multiparticle simulations with up to 50 million particles. To demonstrate the stability of the design matched and mismatched input beams are used.CERN-PS-2001-050-RFCERN-NEUTRINO-FACTORY-NOTE-84CERN-NUFACT-NOTE-84oai:cds.cern.ch:5099862001-07-18
spellingShingle Accelerators and Storage Rings
Gerigk, F
Vretenar, R D
Ryne, M
Design of the Superconducting Section of the SPL LINAC at CERN
title Design of the Superconducting Section of the SPL LINAC at CERN
title_full Design of the Superconducting Section of the SPL LINAC at CERN
title_fullStr Design of the Superconducting Section of the SPL LINAC at CERN
title_full_unstemmed Design of the Superconducting Section of the SPL LINAC at CERN
title_short Design of the Superconducting Section of the SPL LINAC at CERN
title_sort design of the superconducting section of the spl linac at cern
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/509986
work_keys_str_mv AT gerigkf designofthesuperconductingsectionofthespllinacatcern
AT vretenarrd designofthesuperconductingsectionofthespllinacatcern
AT rynem designofthesuperconductingsectionofthespllinacatcern