Cargando…

Luminosity optimisation by adjusting LHC beta* at collision

To correct the beta * at the main collision points (IP1 and IP5) simultaneously for the two counterrotating proton beams in the LHC a set of specific quadrupoles in the non-common part of the machine is used. Due to the antisymmetric optics, several quadrupoles on each side of the insertion have to...

Descripción completa

Detalles Bibliográficos
Autor principal: Wittmer, W
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:http://cds.cern.ch/record/725978
_version_ 1780903732515438592
author Wittmer, W
author_facet Wittmer, W
author_sort Wittmer, W
collection CERN
description To correct the beta * at the main collision points (IP1 and IP5) simultaneously for the two counterrotating proton beams in the LHC a set of specific quadrupoles in the non-common part of the machine is used. Due to the antisymmetric optics, several quadrupoles on each side of the insertion have to be used. The change in the value of beta * is accomplished by changing the k values of the quadrupoles. This set of increments is referred to as beta * tuning knob. The increments were calculated by rematching beta * in a range of +or- 20 % about the nominal value. Linear curves were fitted to the variation of increments to construct a linear tuning knob. This was done for each plane using MAD 8. The linear behaviour and the orthogonality of the knobs were investigated. Different field errors were introduced in the lattice and the correction efficiency of the knobs were studied. (3 refs).
id cern-725978
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
record_format invenio
spelling cern-7259782019-09-30T06:29:59Zhttp://cds.cern.ch/record/725978engWittmer, WLuminosity optimisation by adjusting LHC beta* at collisionAccelerators and Storage RingsTo correct the beta * at the main collision points (IP1 and IP5) simultaneously for the two counterrotating proton beams in the LHC a set of specific quadrupoles in the non-common part of the machine is used. Due to the antisymmetric optics, several quadrupoles on each side of the insertion have to be used. The change in the value of beta * is accomplished by changing the k values of the quadrupoles. This set of increments is referred to as beta * tuning knob. The increments were calculated by rematching beta * in a range of +or- 20 % about the nominal value. Linear curves were fitted to the variation of increments to construct a linear tuning knob. This was done for each plane using MAD 8. The linear behaviour and the orthogonality of the knobs were investigated. Different field errors were introduced in the lattice and the correction efficiency of the knobs were studied. (3 refs).oai:cds.cern.ch:7259782002
spellingShingle Accelerators and Storage Rings
Wittmer, W
Luminosity optimisation by adjusting LHC beta* at collision
title Luminosity optimisation by adjusting LHC beta* at collision
title_full Luminosity optimisation by adjusting LHC beta* at collision
title_fullStr Luminosity optimisation by adjusting LHC beta* at collision
title_full_unstemmed Luminosity optimisation by adjusting LHC beta* at collision
title_short Luminosity optimisation by adjusting LHC beta* at collision
title_sort luminosity optimisation by adjusting lhc beta* at collision
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/725978
work_keys_str_mv AT wittmerw luminosityoptimisationbyadjustinglhcbetaatcollision