Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping

As a part of SPIRAL1 upgrade, several experiments were carried out to understand the transport of 1+ (monocharged) ion beam through the SP1 ECR charge breeder ion source and to investigate the physical processes involved in charge breeding. Ion beam transport simulations were performed to reproduce...

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Main Authors: A. Annaluru, P. Delahaye, M. Dubois, L. Maunoury
Format: Article
Language:English
Published: American Physical Society 2021-07-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.24.073403
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spelling doaj-01bcf6253b7b49fba2ddc84db2d499bd2021-07-30T15:13:31ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882021-07-0124707340310.1103/PhysRevAccelBeams.24.073403Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stoppingA. AnnaluruP. DelahayeM. DuboisL. MaunouryAs a part of SPIRAL1 upgrade, several experiments were carried out to understand the transport of 1+ (monocharged) ion beam through the SP1 ECR charge breeder ion source and to investigate the physical processes involved in charge breeding. Ion beam transport simulations were performed to reproduce the trends of the experimental results (charge breeding efficiency versus 1+ beam injection energy ΔV) by transporting the 1+ beam through a potential map that reflects the presence of the ECR (electron cyclotron resonance) plasma. The role of Coulomb collisions in the capture of 1+ beam leads to a necessary detailed analysis for an accurate description of the charge breeding process. This was done by using a full six-dimensional (6D) phase space Monte Carlo charge breeding (MCBC) code. MCBC models Coulomb collisions of the injected 1+ beam in an ECR plasma and atomic processes (ionization and charge exchange). A simplified background ECR plasma model is implemented in the code to reproduce the trends of three different experiments (interaction of Na^{1+} with He plasma, K^{1+} with He plasma and K^{1+} with O_{2} plasma). The model is able to reproduce the low charge state (1+ and 2+) experimental trends by tuning each plasma parameter (plasma density, plasma ion temperature and electron temperature) independently. The estimated plasma parameters obtained from each case are presented and their contribution in charge breeding process are discussed.http://doi.org/10.1103/PhysRevAccelBeams.24.073403
collection DOAJ
language English
format Article
sources DOAJ
author A. Annaluru
P. Delahaye
M. Dubois
L. Maunoury
spellingShingle A. Annaluru
P. Delahaye
M. Dubois
L. Maunoury
Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping
Physical Review Accelerators and Beams
author_facet A. Annaluru
P. Delahaye
M. Dubois
L. Maunoury
author_sort A. Annaluru
title Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping
title_short Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping
title_full Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping
title_fullStr Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping
title_full_unstemmed Electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping
title_sort electron cyclotron resonance charge breeder plasma parameters from the modeling of 1+ beam stopping
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2021-07-01
description As a part of SPIRAL1 upgrade, several experiments were carried out to understand the transport of 1+ (monocharged) ion beam through the SP1 ECR charge breeder ion source and to investigate the physical processes involved in charge breeding. Ion beam transport simulations were performed to reproduce the trends of the experimental results (charge breeding efficiency versus 1+ beam injection energy ΔV) by transporting the 1+ beam through a potential map that reflects the presence of the ECR (electron cyclotron resonance) plasma. The role of Coulomb collisions in the capture of 1+ beam leads to a necessary detailed analysis for an accurate description of the charge breeding process. This was done by using a full six-dimensional (6D) phase space Monte Carlo charge breeding (MCBC) code. MCBC models Coulomb collisions of the injected 1+ beam in an ECR plasma and atomic processes (ionization and charge exchange). A simplified background ECR plasma model is implemented in the code to reproduce the trends of three different experiments (interaction of Na^{1+} with He plasma, K^{1+} with He plasma and K^{1+} with O_{2} plasma). The model is able to reproduce the low charge state (1+ and 2+) experimental trends by tuning each plasma parameter (plasma density, plasma ion temperature and electron temperature) independently. The estimated plasma parameters obtained from each case are presented and their contribution in charge breeding process are discussed.
url http://doi.org/10.1103/PhysRevAccelBeams.24.073403
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