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Second-order Transit Time Factors for a Two Gap Resonator

The HIE-ISOLDE linac at CERN will operate independently phased quarter-wave resonators (QWRs) in order to accelerate radioactive ion beams (RIBs), with mass to charge states in the range 2.5 < A/q < 4.5, from 1.2 MeV/u up to an energy of at least 10 MeV/u. The low-β version of the QWR will als...

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Autor principal: Fraser, MA
Lenguaje:eng
Publicado: 2009
Materias:
Acceso en línea:http://cds.cern.ch/record/1436066
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author Fraser, MA
author_facet Fraser, MA
author_sort Fraser, MA
collection CERN
description The HIE-ISOLDE linac at CERN will operate independently phased quarter-wave resonators (QWRs) in order to accelerate radioactive ion beams (RIBs), with mass to charge states in the range 2.5 < A/q < 4.5, from 1.2 MeV/u up to an energy of at least 10 MeV/u. The low-β version of the QWR will also be used to decelerate beams below 1.2 MeV/u. The combination of low velocity and high gradient results in a significant change of the ion velocity and a breakdown of the first-order approximation commonly used to calculate the energy gain in accelerating cavities. The first-order transit-time factor for two gaps is briefly reviewed before higher-order transit-time factors are derived and the energy gain expressed, taking into account the variation in velocity, to second-order. The formalism of J.R. Delayen, introduced in [1], is used throughout.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2009
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spelling cern-14360662019-09-30T06:29:59Zhttp://cds.cern.ch/record/1436066engFraser, MASecond-order Transit Time Factors for a Two Gap ResonatorAccelerators and Storage RingsThe HIE-ISOLDE linac at CERN will operate independently phased quarter-wave resonators (QWRs) in order to accelerate radioactive ion beams (RIBs), with mass to charge states in the range 2.5 < A/q < 4.5, from 1.2 MeV/u up to an energy of at least 10 MeV/u. The low-β version of the QWR will also be used to decelerate beams below 1.2 MeV/u. The combination of low velocity and high gradient results in a significant change of the ion velocity and a breakdown of the first-order approximation commonly used to calculate the energy gain in accelerating cavities. The first-order transit-time factor for two gaps is briefly reviewed before higher-order transit-time factors are derived and the energy gain expressed, taking into account the variation in velocity, to second-order. The formalism of J.R. Delayen, introduced in [1], is used throughout.HIE-ISOLDE-PROJECT-Note-0005CERN-BE-2009-RFCERN-HIE-ISOLDE-PROJECT-Note-0005oai:cds.cern.ch:14360662009-10-01
spellingShingle Accelerators and Storage Rings
Fraser, MA
Second-order Transit Time Factors for a Two Gap Resonator
title Second-order Transit Time Factors for a Two Gap Resonator
title_full Second-order Transit Time Factors for a Two Gap Resonator
title_fullStr Second-order Transit Time Factors for a Two Gap Resonator
title_full_unstemmed Second-order Transit Time Factors for a Two Gap Resonator
title_short Second-order Transit Time Factors for a Two Gap Resonator
title_sort second-order transit time factors for a two gap resonator
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/1436066
work_keys_str_mv AT fraserma secondordertransittimefactorsforatwogapresonator