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CTF3 Drive Beam Injector Optimisation

In the Compact Linear Collider (CLIC) the RF power for the acceleration of the Main Beam is extracted from a high-current Drive Beam that runs parallel to the main linac. The main feasibility issues of the two-beam acceleration scheme are being demonstrated at CLIC Test Facility 3 (CTF3). The CTF3 D...

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Autores principales: Sanaye Hajari, Shahin, Shaker, H, Doebert, S
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:http://cds.cern.ch/record/2119551
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author Sanaye Hajari, Shahin
Shaker, H
Doebert, S
author_facet Sanaye Hajari, Shahin
Shaker, H
Doebert, S
author_sort Sanaye Hajari, Shahin
collection CERN
description In the Compact Linear Collider (CLIC) the RF power for the acceleration of the Main Beam is extracted from a high-current Drive Beam that runs parallel to the main linac. The main feasibility issues of the two-beam acceleration scheme are being demonstrated at CLIC Test Facility 3 (CTF3). The CTF3 Drive Beam injector consists of a thermionic gun followed by the bunching system and two accelerating structures all embedded in solenoidal magnetic field and a magnetic chicane. Three sub-harmonic bunchers (SHB), a prebuncher and a travelling wave buncher constitute the bunching system. The phase coding process done by the sub-harmonic bunching system produces unwanted satellite bunches between the successive main bunches. The beam dynamics of the CTF3 Drive Beam injector is reoptimised with the goal of improving the injector performance and in particular decreasing the satellite population, the beam loss in the magnetic chicane and the beam emittance in transverse plane compare to the original model based on P. Urschuetz works.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2015
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spelling cern-21195512023-07-20T15:07:14Zhttp://cds.cern.ch/record/2119551engSanaye Hajari, ShahinShaker, HDoebert, SCTF3 Drive Beam Injector OptimisationAccelerators and Storage RingsIn the Compact Linear Collider (CLIC) the RF power for the acceleration of the Main Beam is extracted from a high-current Drive Beam that runs parallel to the main linac. The main feasibility issues of the two-beam acceleration scheme are being demonstrated at CLIC Test Facility 3 (CTF3). The CTF3 Drive Beam injector consists of a thermionic gun followed by the bunching system and two accelerating structures all embedded in solenoidal magnetic field and a magnetic chicane. Three sub-harmonic bunchers (SHB), a prebuncher and a travelling wave buncher constitute the bunching system. The phase coding process done by the sub-harmonic bunching system produces unwanted satellite bunches between the successive main bunches. The beam dynamics of the CTF3 Drive Beam injector is reoptimised with the goal of improving the injector performance and in particular decreasing the satellite population, the beam loss in the magnetic chicane and the beam emittance in transverse plane compare to the original model based on P. Urschuetz works.CERN-ACC-2016-0002CLIC-Note-1060oai:cds.cern.ch:21195512015-06-30
spellingShingle Accelerators and Storage Rings
Sanaye Hajari, Shahin
Shaker, H
Doebert, S
CTF3 Drive Beam Injector Optimisation
title CTF3 Drive Beam Injector Optimisation
title_full CTF3 Drive Beam Injector Optimisation
title_fullStr CTF3 Drive Beam Injector Optimisation
title_full_unstemmed CTF3 Drive Beam Injector Optimisation
title_short CTF3 Drive Beam Injector Optimisation
title_sort ctf3 drive beam injector optimisation
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/2119551
work_keys_str_mv AT sanayehajarishahin ctf3drivebeaminjectoroptimisation
AT shakerh ctf3drivebeaminjectoroptimisation
AT doeberts ctf3drivebeaminjectoroptimisation