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Beam Dynamics in the LINAC4/SPL CCDTL

The Cell-Coupled DTL section of the LINAC4/SPL is designed to accelerate H- ions from 40 MeV up to 90 MeV energy and is situated downstream the Alvarez DTL. Following the change in the original acceleration range of 40-120 MeV to 40-90 MeV and some RF design changes in the Alvarez DTL, the RF and be...

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Detalles Bibliográficos
Autores principales: Sargsyan, E, Lombardi, A
Lenguaje:eng
Publicado: 2005
Materias:
Acceso en línea:http://cds.cern.ch/record/855450
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author Sargsyan, E
Lombardi, A
author_facet Sargsyan, E
Lombardi, A
author_sort Sargsyan, E
collection CERN
description The Cell-Coupled DTL section of the LINAC4/SPL is designed to accelerate H- ions from 40 MeV up to 90 MeV energy and is situated downstream the Alvarez DTL. Following the change in the original acceleration range of 40-120 MeV to 40-90 MeV and some RF design changes in the Alvarez DTL, the RF and beam dynamics designs of the CCDTL have been revised. The present note deals with the beam dynamics design of the new CCDTL layout. The end-to-end beam dynamics in the Alvarez DTL+CCDTL is presented as well. The beam dynamics design is based on avoiding emittance exchange between the longitudinal and the transverse planes due to the space-charge resonance that would lead to an emittance growth and consequently to a beam losses.
id cern-855450
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2005
record_format invenio
spelling cern-8554502019-09-30T06:29:59Zhttp://cds.cern.ch/record/855450engSargsyan, ELombardi, ABeam Dynamics in the LINAC4/SPL CCDTLAccelerators and Storage RingsThe Cell-Coupled DTL section of the LINAC4/SPL is designed to accelerate H- ions from 40 MeV up to 90 MeV energy and is situated downstream the Alvarez DTL. Following the change in the original acceleration range of 40-120 MeV to 40-90 MeV and some RF design changes in the Alvarez DTL, the RF and beam dynamics designs of the CCDTL have been revised. The present note deals with the beam dynamics design of the new CCDTL layout. The end-to-end beam dynamics in the Alvarez DTL+CCDTL is presented as well. The beam dynamics design is based on avoiding emittance exchange between the longitudinal and the transverse planes due to the space-charge resonance that would lead to an emittance growth and consequently to a beam losses.AB-Note-2005-032CERN-AB-Note-2005-032oai:cds.cern.ch:8554502005-09-20
spellingShingle Accelerators and Storage Rings
Sargsyan, E
Lombardi, A
Beam Dynamics in the LINAC4/SPL CCDTL
title Beam Dynamics in the LINAC4/SPL CCDTL
title_full Beam Dynamics in the LINAC4/SPL CCDTL
title_fullStr Beam Dynamics in the LINAC4/SPL CCDTL
title_full_unstemmed Beam Dynamics in the LINAC4/SPL CCDTL
title_short Beam Dynamics in the LINAC4/SPL CCDTL
title_sort beam dynamics in the linac4/spl ccdtl
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/855450
work_keys_str_mv AT sargsyane beamdynamicsinthelinac4splccdtl
AT lombardia beamdynamicsinthelinac4splccdtl