Cargando…

The transverse and longitudinal beam characteristics of the PHIN photo-injector at CERN

A new photo-injector, capable to deliver a long pulse train with a high charge per bunch for CTF3, has been designed and installed by a collaboration between LAL, CCLRC and CERN within the framework of the second Joint Research Activity PHIN of the European CARE program. The demonstration of the hig...

Descripción completa

Detalles Bibliográficos
Autores principales: Mete, Ö, Chevallay, E, Dabrowski, A, Divall, M, Döbert, S, Egger, D, Elsener, K, Fedosseev, V, Lefèvre, T, Petrarca, M
Lenguaje:eng
Publicado: 2010
Materias:
Acceso en línea:http://cds.cern.ch/record/1262856
_version_ 1780920009381380096
author Mete, Ö
Chevallay, E
Dabrowski, A
Divall, M
Döbert, S
Egger, D
Elsener, K
Fedosseev, V
Lefèvre, T
Petrarca, M
author_facet Mete, Ö
Chevallay, E
Dabrowski, A
Divall, M
Döbert, S
Egger, D
Elsener, K
Fedosseev, V
Lefèvre, T
Petrarca, M
author_sort Mete, Ö
collection CERN
description A new photo-injector, capable to deliver a long pulse train with a high charge per bunch for CTF3, has been designed and installed by a collaboration between LAL, CCLRC and CERN within the framework of the second Joint Research Activity PHIN of the European CARE program. The demonstration of the high charge and the stability along the pulse train are the important goals for CTF3 and the CLIC drive beam. The nominal beam for CTF3 has an average current of 3.5 A, a 1.5 GHz bunch repetation frequency and a pulse length of 1.27 μs (1908 bunches). The existing CTF3 injector consists of a thermionic gun and a subharmonic bunching system. The PHIN photo-injector is being tested in a dedicated test-stand at CERN to replace the existing CTF3 injector that is producing unwanted satellite bunches during the bunching process. A phase-coding scheme is planned to be implemented to the PHIN laser system providing the required beam temporal structure by CTF3. RF photo-injectors are high-brightness, low-emittance electron sources. One of the main beam dynamics issues for a high brightness electron source, is the optimization of beam envelope behavior in the presence of the space charge force in order to control the beam emittance. Beam based measurements, such as single shot emittance measurement with a multi-slit configuration, have been performed during the commissioning runs in 2008 and 2009. In this work the photo-injector will be describe d and the first beam test results will be presented and compared with simulations.
id cern-1262856
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2010
record_format invenio
spelling cern-12628562023-07-20T15:05:18Zhttp://cds.cern.ch/record/1262856engMete, ÖChevallay, EDabrowski, ADivall, MDöbert, SEgger, DElsener, KFedosseev, VLefèvre, TPetrarca, MThe transverse and longitudinal beam characteristics of the PHIN photo-injector at CERNAccelerators and Storage RingsA new photo-injector, capable to deliver a long pulse train with a high charge per bunch for CTF3, has been designed and installed by a collaboration between LAL, CCLRC and CERN within the framework of the second Joint Research Activity PHIN of the European CARE program. The demonstration of the high charge and the stability along the pulse train are the important goals for CTF3 and the CLIC drive beam. The nominal beam for CTF3 has an average current of 3.5 A, a 1.5 GHz bunch repetation frequency and a pulse length of 1.27 μs (1908 bunches). The existing CTF3 injector consists of a thermionic gun and a subharmonic bunching system. The PHIN photo-injector is being tested in a dedicated test-stand at CERN to replace the existing CTF3 injector that is producing unwanted satellite bunches during the bunching process. A phase-coding scheme is planned to be implemented to the PHIN laser system providing the required beam temporal structure by CTF3. RF photo-injectors are high-brightness, low-emittance electron sources. One of the main beam dynamics issues for a high brightness electron source, is the optimization of beam envelope behavior in the presence of the space charge force in order to control the beam emittance. Beam based measurements, such as single shot emittance measurement with a multi-slit configuration, have been performed during the commissioning runs in 2008 and 2009. In this work the photo-injector will be describe d and the first beam test results will be presented and compared with simulations.CERN-OPEN-2010-013CLIC-Note-809oai:cds.cern.ch:12628562010-03-22
spellingShingle Accelerators and Storage Rings
Mete, Ö
Chevallay, E
Dabrowski, A
Divall, M
Döbert, S
Egger, D
Elsener, K
Fedosseev, V
Lefèvre, T
Petrarca, M
The transverse and longitudinal beam characteristics of the PHIN photo-injector at CERN
title The transverse and longitudinal beam characteristics of the PHIN photo-injector at CERN
title_full The transverse and longitudinal beam characteristics of the PHIN photo-injector at CERN
title_fullStr The transverse and longitudinal beam characteristics of the PHIN photo-injector at CERN
title_full_unstemmed The transverse and longitudinal beam characteristics of the PHIN photo-injector at CERN
title_short The transverse and longitudinal beam characteristics of the PHIN photo-injector at CERN
title_sort transverse and longitudinal beam characteristics of the phin photo-injector at cern
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/1262856
work_keys_str_mv AT meteo thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT chevallaye thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT dabrowskia thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT divallm thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT doberts thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT eggerd thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT elsenerk thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT fedosseevv thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT lefevret thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT petrarcam thetransverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT meteo transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT chevallaye transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT dabrowskia transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT divallm transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT doberts transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT eggerd transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT elsenerk transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT fedosseevv transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT lefevret transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern
AT petrarcam transverseandlongitudinalbeamcharacteristicsofthephinphotoinjectoratcern