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The LHC IR6 optics

The IR6 insertion houses the LHC beam dumping system. Large drift spaces are provided to accommodate the kicker and septum for the beam extraction and to minimise the strength of these components. This implies large values of the B-functions and associated constraints on the aperture of the componen...

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Autor principal: Verdier, A
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:http://cds.cern.ch/record/691998
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author Verdier, A
author_facet Verdier, A
author_sort Verdier, A
collection CERN
description The IR6 insertion houses the LHC beam dumping system. Large drift spaces are provided to accommodate the kicker and septum for the beam extraction and to minimise the strength of these components. This implies large values of the B-functions and associated constraints on the aperture of the components of the beam dump system. The design of these components has been made according to prelim inary versions of the LHC optics. Their characteristics have now to be taken as boundary conditions for the optics. Version 5 of the LHC optics was made with a new dispersion suppressor allowin g at least four different values of the tune-split. The possible variations of the phase advances of the insertion were exhaustively studied for the tunes {Qx=63, Qy=59} and checked for {Qx=66, Qy= 58}, the largest tune split up to now. The aperture constraints associated with the present design of the kicker and septum can be fulfilled. The old Q6 and Q7 are no longer needed, which makes a saving of 10 quadrupoles. The gradient requirements on the insertion and suppressor quadrupoles are given.
id cern-691998
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1998
record_format invenio
spelling cern-6919982023-05-31T13:25:20Zhttp://cds.cern.ch/record/691998engVerdier, AThe LHC IR6 opticsAccelerators and Storage RingsThe IR6 insertion houses the LHC beam dumping system. Large drift spaces are provided to accommodate the kicker and septum for the beam extraction and to minimise the strength of these components. This implies large values of the B-functions and associated constraints on the aperture of the components of the beam dump system. The design of these components has been made according to prelim inary versions of the LHC optics. Their characteristics have now to be taken as boundary conditions for the optics. Version 5 of the LHC optics was made with a new dispersion suppressor allowin g at least four different values of the tune-split. The possible variations of the phase advances of the insertion were exhaustively studied for the tunes {Qx=63, Qy=59} and checked for {Qx=66, Qy= 58}, the largest tune split up to now. The aperture constraints associated with the present design of the kicker and septum can be fulfilled. The old Q6 and Q7 are no longer needed, which makes a saving of 10 quadrupoles. The gradient requirements on the insertion and suppressor quadrupoles are given.LHC-Project-Note-146oai:cds.cern.ch:6919981998-06-29
spellingShingle Accelerators and Storage Rings
Verdier, A
The LHC IR6 optics
title The LHC IR6 optics
title_full The LHC IR6 optics
title_fullStr The LHC IR6 optics
title_full_unstemmed The LHC IR6 optics
title_short The LHC IR6 optics
title_sort lhc ir6 optics
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/691998
work_keys_str_mv AT verdiera thelhcir6optics
AT verdiera lhcir6optics