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Chapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimators

In Run 3 the intensity of the ion beams (usually Pb ions) for ion–ion collisions is planned to be increased by a factor of three: from 40 × 109 to 120 × 109 circulating particles. This intensity increase will amplify the losses in the cold zone at P2 and P7 and may drive the beam induced heat losses...

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Detalles Bibliográficos
Autores principales: Savary, Frederic, Schoerling, Daniel
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.23731/CYRM-2020-0010.213
http://cds.cern.ch/record/2750426
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author Savary, Frederic
Schoerling, Daniel
author_facet Savary, Frederic
Schoerling, Daniel
author_sort Savary, Frederic
collection CERN
description In Run 3 the intensity of the ion beams (usually Pb ions) for ion–ion collisions is planned to be increased by a factor of three: from 40 × 109 to 120 × 109 circulating particles. This intensity increase will amplify the losses in the cold zone at P2 and P7 and may drive the beam induced heat losses in the main dipoles in the dispersion suppressor (DS) region above the quench limit. To avoid limiting the machine performance during ion operation due to this effect, various countermeasures have been studied, and the solution chosen was to intercept these diffractive losses via warm absorbers, so-called TCLDs (Target Collimator Long Dispersion) suppressors, left and right of the LHC interaction points P2 and P7.
id oai-inspirehep.net-1842572
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2020
record_format invenio
spelling oai-inspirehep.net-18425722021-03-24T14:07:19Zdoi:10.23731/CYRM-2020-0010.213http://cds.cern.ch/record/2750426engSavary, FredericSchoerling, DanielChapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimatorsAccelerators and Storage RingsIn Run 3 the intensity of the ion beams (usually Pb ions) for ion–ion collisions is planned to be increased by a factor of three: from 40 × 109 to 120 × 109 circulating particles. This intensity increase will amplify the losses in the cold zone at P2 and P7 and may drive the beam induced heat losses in the main dipoles in the dispersion suppressor (DS) region above the quench limit. To avoid limiting the machine performance during ion operation due to this effect, various countermeasures have been studied, and the solution chosen was to intercept these diffractive losses via warm absorbers, so-called TCLDs (Target Collimator Long Dispersion) suppressors, left and right of the LHC interaction points P2 and P7.oai:inspirehep.net:18425722020
spellingShingle Accelerators and Storage Rings
Savary, Frederic
Schoerling, Daniel
Chapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimators
title Chapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimators
title_full Chapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimators
title_fullStr Chapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimators
title_full_unstemmed Chapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimators
title_short Chapter 11: 11 T dipole and new connection cryostat for the dispersion suppressor collimators
title_sort chapter 11: 11 t dipole and new connection cryostat for the dispersion suppressor collimators
topic Accelerators and Storage Rings
url https://dx.doi.org/10.23731/CYRM-2020-0010.213
http://cds.cern.ch/record/2750426
work_keys_str_mv AT savaryfrederic chapter1111tdipoleandnewconnectioncryostatforthedispersionsuppressorcollimators
AT schoerlingdaniel chapter1111tdipoleandnewconnectioncryostatforthedispersionsuppressorcollimators