Effect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle Tracking

Linac4 is a 160 MeV H- linear accelerator which will replace the 50 MeV proton Linac2 for upgrade of the LHC injectors with higher intensity and eventually an increase of the LHC luminosity. Linac4 structure is a source, a 45 keV low energy beam transport line (LEBT) with two solenoids, a 3 MeV Radi...

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Detalles Bibliográficos
Autores principales: Yarmohammadi Satri, M, Lombardi, A
Lenguaje:eng
Publicado: 2013
Materias:
Accelerators and Storage Rings
Acceso en línea:http://cds.cern.ch/record/1612506
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author Yarmohammadi Satri, M
Lombardi, A
author_facet Yarmohammadi Satri, M
Lombardi, A
author_sort Yarmohammadi Satri, M
collection CERN
description Linac4 is a 160 MeV H- linear accelerator which will replace the 50 MeV proton Linac2 for upgrade of the LHC injectors with higher intensity and eventually an increase of the LHC luminosity. Linac4 structure is a source, a 45 keV low energy beam transport line (LEBT) with two solenoids, a 3 MeV Radiofrequency Quadrupole (RFQ), a Medium Energy Beam Transport line (MEBT), a 50 Mev DTL, a 100 Mev CCDTL and PIMS up to 160 Mev. We use Travel v4.07 and PathManager code for simulation. Firstly, we need to a file as a source and defining the beginning point (last point in tracking back) of simulation. We recognise the starting point base on the solenoid magnetic property of LEBT.
id cern-1612506
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2013
record_format invenio
spelling cern-16125062023-08-04T20:24:59Zhttp://cds.cern.ch/record/1612506engYarmohammadi Satri, MLombardi, AEffect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle TrackingAccelerators and Storage RingsLinac4 is a 160 MeV H- linear accelerator which will replace the 50 MeV proton Linac2 for upgrade of the LHC injectors with higher intensity and eventually an increase of the LHC luminosity. Linac4 structure is a source, a 45 keV low energy beam transport line (LEBT) with two solenoids, a 3 MeV Radiofrequency Quadrupole (RFQ), a Medium Energy Beam Transport line (MEBT), a 50 Mev DTL, a 100 Mev CCDTL and PIMS up to 160 Mev. We use Travel v4.07 and PathManager code for simulation. Firstly, we need to a file as a source and defining the beginning point (last point in tracking back) of simulation. We recognise the starting point base on the solenoid magnetic property of LEBT.CERN-ACC-Note-2013-0029oai:cds.cern.ch:16125062013-10-21
spellingShingle Accelerators and Storage Rings
Yarmohammadi Satri, M
Lombardi, A
Effect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle Tracking
title Effect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle Tracking
title_full Effect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle Tracking
title_fullStr Effect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle Tracking
title_full_unstemmed Effect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle Tracking
title_short Effect Of The LEBT Solenoid Magnetic Field On The Beam Generation For Particle Tracking
title_sort effect of the lebt solenoid magnetic field on the beam generation for particle tracking
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/1612506
work_keys_str_mv AT yarmohammadisatrim effectofthelebtsolenoidmagneticfieldonthebeamgenerationforparticletracking
AT lombardia effectofthelebtsolenoidmagneticfieldonthebeamgenerationforparticletracking

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