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Beam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV)
After the decomissioning of LEP-2 a considerable amount of RF hardware becomes available and can be used for the construction of a high current superconducting proton linac [1]. The present design of the SPL uses four types of superconducting cavities (beta=0.52, 0.7, 0.8, and LEP) to accelerate a p...
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Lenguaje: | eng |
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2000
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Acceso en línea: | http://cds.cern.ch/record/479867 |
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author | Gerigk, F |
author_facet | Gerigk, F |
author_sort | Gerigk, F |
collection | CERN |
description | After the decomissioning of LEP-2 a considerable amount of RF hardware becomes available and can be used for the construction of a high current superconducting proton linac [1]. The present design of the SPL uses four types of superconducting cavities (beta=0.52, 0.7, 0.8, and LEP) to accelerate a pulsed beam of 70 mA from 120 MeV up to 2.2 GeV. In this paper a beam dynamics layout for the superconducting section is presented. The layout is optimized to keep the overall linac length short and to ensure a stable steering of the beam. Multiparticle simulations have been carried out to analyse the proposed focusing structure, and to investigate emittance growth for the nominal case and for a mismatched input beam. |
id | cern-479867 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2000 |
record_format | invenio |
spelling | cern-4798672023-06-23T09:22:48Zhttp://cds.cern.ch/record/479867engGerigk, FBeam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV)Accelerators and Storage RingsAfter the decomissioning of LEP-2 a considerable amount of RF hardware becomes available and can be used for the construction of a high current superconducting proton linac [1]. The present design of the SPL uses four types of superconducting cavities (beta=0.52, 0.7, 0.8, and LEP) to accelerate a pulsed beam of 70 mA from 120 MeV up to 2.2 GeV. In this paper a beam dynamics layout for the superconducting section is presented. The layout is optimized to keep the overall linac length short and to ensure a stable steering of the beam. Multiparticle simulations have been carried out to analyse the proposed focusing structure, and to investigate emittance growth for the nominal case and for a mismatched input beam.CERN-OPEN-2000-331CERN-NEUTRINO-FACTORY-NOTE-24CERN-NUFACT-NOTE-24CERN-PS-RF-Note-009-00CERN-PS-RF-Note-2000-009oai:cds.cern.ch:4798672000-03-15 |
spellingShingle | Accelerators and Storage Rings Gerigk, F Beam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV) |
title | Beam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV) |
title_full | Beam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV) |
title_fullStr | Beam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV) |
title_full_unstemmed | Beam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV) |
title_short | Beam Dynamics in the Superconducting Section of the SPL (120 MeV - 2.2 GeV) |
title_sort | beam dynamics in the superconducting section of the spl (120 mev - 2.2 gev) |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/479867 |
work_keys_str_mv | AT gerigkf beamdynamicsinthesuperconductingsectionofthespl120mev22gev |