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A procedure for obtaining transverse wall impedance and working line from transfer function measurements

In order to measure the variation of betatron tune versus momentum, the 'working line', the effect of the wall impedance must be eliminated. The method is based on a comparison between the longitudinal particle distribution calculated from the transfer function of a slow and a fast wave, a...

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Detalles Bibliográficos
Autores principales: Hémery, J Y, Vos, L
Lenguaje:eng
Publicado: 1980
Materias:
Acceso en línea:http://cds.cern.ch/record/879239
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author Hémery, J Y
Vos, L
author_facet Hémery, J Y
Vos, L
author_sort Hémery, J Y
collection CERN
description In order to measure the variation of betatron tune versus momentum, the 'working line', the effect of the wall impedance must be eliminated. The method is based on a comparison between the longitudinal particle distribution calculated from the transfer function of a slow and a fast wave, and the measured longitudinal distribution. The difference between the two is due to the transverse wall impedance. A matching routine yields the correct longitudinal and betatron distributions, the working line and the stability diagram. However, the data have to be treated prior to this operation to eliminate a number of parasitic effects in order to ensure a sufficient precision. The results of the method are presented.
id cern-879239
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1980
record_format invenio
spelling cern-8792392023-04-21T09:45:10Zhttp://cds.cern.ch/record/879239engHémery, J YVos, LA procedure for obtaining transverse wall impedance and working line from transfer function measurementsAccelerators and Storage RingsIn order to measure the variation of betatron tune versus momentum, the 'working line', the effect of the wall impedance must be eliminated. The method is based on a comparison between the longitudinal particle distribution calculated from the transfer function of a slow and a fast wave, and the measured longitudinal distribution. The difference between the two is due to the transverse wall impedance. A matching routine yields the correct longitudinal and betatron distributions, the working line and the stability diagram. However, the data have to be treated prior to this operation to eliminate a number of parasitic effects in order to ensure a sufficient precision. The results of the method are presented.CERN-ISR-CO-OP-80-32ISR-CO-OP-80-32oai:cds.cern.ch:8792391980
spellingShingle Accelerators and Storage Rings
Hémery, J Y
Vos, L
A procedure for obtaining transverse wall impedance and working line from transfer function measurements
title A procedure for obtaining transverse wall impedance and working line from transfer function measurements
title_full A procedure for obtaining transverse wall impedance and working line from transfer function measurements
title_fullStr A procedure for obtaining transverse wall impedance and working line from transfer function measurements
title_full_unstemmed A procedure for obtaining transverse wall impedance and working line from transfer function measurements
title_short A procedure for obtaining transverse wall impedance and working line from transfer function measurements
title_sort procedure for obtaining transverse wall impedance and working line from transfer function measurements
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/879239
work_keys_str_mv AT hemeryjy aprocedureforobtainingtransversewallimpedanceandworkinglinefromtransferfunctionmeasurements
AT vosl aprocedureforobtainingtransversewallimpedanceandworkinglinefromtransferfunctionmeasurements
AT hemeryjy procedureforobtainingtransversewallimpedanceandworkinglinefromtransferfunctionmeasurements
AT vosl procedureforobtainingtransversewallimpedanceandworkinglinefromtransferfunctionmeasurements