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Distribution of the RF System in a Very Large Lepton Collider

The consequences for the beam dynamics are discussed of concentrating the radio-frequency accelerating system of a very large circular e+e- collider VLLC in a few places around the circumference. As specific example, a VLLC with four long straight sections with RF systems and possibly interaction po...

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Autor principal: Keil, Eberhard
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:http://cds.cern.ch/record/702654
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author Keil, Eberhard
author_facet Keil, Eberhard
author_sort Keil, Eberhard
collection CERN
description The consequences for the beam dynamics are discussed of concentrating the radio-frequency accelerating system of a very large circular e+e- collider VLLC in a few places around the circumference. As specific example, a VLLC with four long straight sections with RF systems and possibly interaction points and four arcs is used. At 184 GeV beam energy, each RF system accelerates the two beams by about 1 GeV, and causes energy variations between +/- 0.27 % around the circumference. By arranging the RF systems symmetrically around the interaction points, the centre-of-mass energies there are all equal to twice the beam energy. In a VLLC model without low-beta insertions, the effects of this sawtooth energy variation on the mismatch of the horizontal orbit and dispersion, and the amplitude functions are all rather small.
id cern-702654
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
record_format invenio
spelling cern-7026542023-05-11T12:03:33Zhttp://cds.cern.ch/record/702654engKeil, EberhardDistribution of the RF System in a Very Large Lepton ColliderAccelerators and Storage RingsThe consequences for the beam dynamics are discussed of concentrating the radio-frequency accelerating system of a very large circular e+e- collider VLLC in a few places around the circumference. As specific example, a VLLC with four long straight sections with RF systems and possibly interaction points and four arcs is used. At 184 GeV beam energy, each RF system accelerates the two beams by about 1 GeV, and causes energy variations between +/- 0.27 % around the circumference. By arranging the RF systems symmetrically around the interaction points, the centre-of-mass energies there are all equal to twice the beam energy. In a VLLC model without low-beta insertions, the effects of this sawtooth energy variation on the mismatch of the horizontal orbit and dispersion, and the amplitude functions are all rather small.SL-Note-2001-019-APoai:cds.cern.ch:7026542001-04-24
spellingShingle Accelerators and Storage Rings
Keil, Eberhard
Distribution of the RF System in a Very Large Lepton Collider
title Distribution of the RF System in a Very Large Lepton Collider
title_full Distribution of the RF System in a Very Large Lepton Collider
title_fullStr Distribution of the RF System in a Very Large Lepton Collider
title_full_unstemmed Distribution of the RF System in a Very Large Lepton Collider
title_short Distribution of the RF System in a Very Large Lepton Collider
title_sort distribution of the rf system in a very large lepton collider
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/702654
work_keys_str_mv AT keileberhard distributionoftherfsysteminaverylargeleptoncollider