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Injection and acceleration with physics optics in LEP

Up to now injection into LEP has been done using a dedicated injection optics, with a vertical b*v = 21 cm. After accelerating to higher energies a progressive optics change is made with beam to the Œphysics¹ optics, where b*v = 5 cm. The use of synchrotron injection as the normal means of accumulat...

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Detalles Bibliográficos
Autores principales: Collier, Paul, Roy, G
Lenguaje:eng
Publicado: 1996
Materias:
Acceso en línea:http://cds.cern.ch/record/306914
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author Collier, Paul
Roy, G
author_facet Collier, Paul
Roy, G
author_sort Collier, Paul
collection CERN
description Up to now injection into LEP has been done using a dedicated injection optics, with a vertical b*v = 21 cm. After accelerating to higher energies a progressive optics change is made with beam to the Œphysics¹ optics, where b*v = 5 cm. The use of synchrotron injection as the normal means of accumulation in LEP has opened up the possibility of injecting directly into the Œphysics¹ optics. This has many advantages ranging from an easier operation, including a faster turnaround from injection to physics conditions, to allowing more flexibility in the optics design and matching. Results from machine development sessions are presented showing that there is no fundamental reason for not implementing this scheme. Potential drawbacks and limitations, especially for the maximum accumulated beam current are, however, discussed.
id cern-306914
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1996
record_format invenio
spelling cern-3069142023-05-05T12:57:25Zhttp://cds.cern.ch/record/306914engCollier, PaulRoy, GInjection and acceleration with physics optics in LEPAccelerators and Storage RingsUp to now injection into LEP has been done using a dedicated injection optics, with a vertical b*v = 21 cm. After accelerating to higher energies a progressive optics change is made with beam to the Œphysics¹ optics, where b*v = 5 cm. The use of synchrotron injection as the normal means of accumulation in LEP has opened up the possibility of injecting directly into the Œphysics¹ optics. This has many advantages ranging from an easier operation, including a faster turnaround from injection to physics conditions, to allowing more flexibility in the optics design and matching. Results from machine development sessions are presented showing that there is no fundamental reason for not implementing this scheme. Potential drawbacks and limitations, especially for the maximum accumulated beam current are, however, discussed.CERN-SL-96-020-OPoai:cds.cern.ch:3069141996-06-26
spellingShingle Accelerators and Storage Rings
Collier, Paul
Roy, G
Injection and acceleration with physics optics in LEP
title Injection and acceleration with physics optics in LEP
title_full Injection and acceleration with physics optics in LEP
title_fullStr Injection and acceleration with physics optics in LEP
title_full_unstemmed Injection and acceleration with physics optics in LEP
title_short Injection and acceleration with physics optics in LEP
title_sort injection and acceleration with physics optics in lep
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/306914
work_keys_str_mv AT collierpaul injectionandaccelerationwithphysicsopticsinlep
AT royg injectionandaccelerationwithphysicsopticsinlep