Cargando…

Correcting the 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 Large Hadron Collider (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 o...

Descripción completa

Detalles Bibliográficos
Autores principales: Verdier, A, Wittmer, W, Zimmermann, Frank
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:http://cds.cern.ch/record/620196
_version_ 1780900375756275712
author Verdier, A
Wittmer, W
Zimmermann, Frank
author_facet Verdier, A
Wittmer, W
Zimmermann, Frank
author_sort Verdier, A
collection CERN
description To correct the beta* at the main collision points (IP1 and IP5) simultaneously for the two counterrotating proton beams in the Large Hadron Collider (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 employed. The change of beta* is accomplished by incrementing the quadrupole gradients. This set of increments is referred to as beta* tuning knob. The increments were calculated by rematching beta* in a range of + 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 [1] and repeated with MAD X [2]. The linear behaviour and the orthogonality of the knobs were investigated for the LHC lattices V6.2 and V6.4. Different field errors were introduced in the lattice and the correction efficiency of the knobs was studied.
id cern-620196
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2003
record_format invenio
spelling cern-6201962023-05-31T13:24:02Zhttp://cds.cern.ch/record/620196engVerdier, AWittmer, WZimmermann, FrankCorrecting the 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 Large Hadron Collider (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 employed. The change of beta* is accomplished by incrementing the quadrupole gradients. This set of increments is referred to as beta* tuning knob. The increments were calculated by rematching beta* in a range of + 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 [1] and repeated with MAD X [2]. The linear behaviour and the orthogonality of the knobs were investigated for the LHC lattices V6.2 and V6.4. Different field errors were introduced in the lattice and the correction efficiency of the knobs was studied.LHC-Project-Report-647CERN-LHC-Project-Report-647oai:cds.cern.ch:6201962003-06-05
spellingShingle Accelerators and Storage Rings
Verdier, A
Wittmer, W
Zimmermann, Frank
Correcting the LHC beta* at Collision
title Correcting the LHC beta* at Collision
title_full Correcting the LHC beta* at Collision
title_fullStr Correcting the LHC beta* at Collision
title_full_unstemmed Correcting the LHC beta* at Collision
title_short Correcting the LHC beta* at Collision
title_sort correcting the lhc beta* at collision
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/620196
work_keys_str_mv AT verdiera correctingthelhcbetaatcollision
AT wittmerw correctingthelhcbetaatcollision
AT zimmermannfrank correctingthelhcbetaatcollision