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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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Lenguaje: | eng |
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2009
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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. |
id | cern-1436066 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2009 |
record_format | invenio |
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 |