Model of charge-state distributions for electron cyclotron resonance ion source plasmas

A computer model for the ion charge-state distribution (CSD) in an electron cyclotron resonance ion source (ECRIS) plasma is presented that incorporates non-Maxwellian distribution functions, multiple atomic species, and ion confinement due to the ambipolar potential well that arises from confinemen...

Full description

Bibliographic Details
Main Authors: D. H. Edgell, J. S. Kim, S. K. Wong, R. C. Pardo, R. Vondrasek
Format: Article
Language:English
Published: American Physical Society 1999-12-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.2.123502
id doaj-47838c34c7764351994a8d1833752391
record_format Article
spelling doaj-47838c34c7764351994a8d18337523912020-11-24T21:26:29ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44021999-12-0121212350210.1103/PhysRevSTAB.2.123502Model of charge-state distributions for electron cyclotron resonance ion source plasmasD. H. EdgellJ. S. KimS. K. WongR. C. PardoR. VondrasekA computer model for the ion charge-state distribution (CSD) in an electron cyclotron resonance ion source (ECRIS) plasma is presented that incorporates non-Maxwellian distribution functions, multiple atomic species, and ion confinement due to the ambipolar potential well that arises from confinement of the electron cyclotron resonance (ECR) heated electrons. Atomic processes incorporated into the model include multiple ionization and multiple charge exchange with rate coefficients calculated for non-Maxwellian electron distributions. The electron distribution function is calculated using a Fokker-Planck code with an ECR heating term. This eliminates the electron temperature as an arbitrary user input. The model produces results that are a good match to CSD data from the ANL-ECRII ECRIS. Extending the model to 1D axial will also allow the model to determine the plasma and electrostatic potential profiles, further eliminating arbitrary user input to the model.http://doi.org/10.1103/PhysRevSTAB.2.123502
collection DOAJ
language English
format Article
sources DOAJ
author D. H. Edgell
J. S. Kim
S. K. Wong
R. C. Pardo
R. Vondrasek
spellingShingle D. H. Edgell
J. S. Kim
S. K. Wong
R. C. Pardo
R. Vondrasek
Model of charge-state distributions for electron cyclotron resonance ion source plasmas
Physical Review Special Topics. Accelerators and Beams
author_facet D. H. Edgell
J. S. Kim
S. K. Wong
R. C. Pardo
R. Vondrasek
author_sort D. H. Edgell
title Model of charge-state distributions for electron cyclotron resonance ion source plasmas
title_short Model of charge-state distributions for electron cyclotron resonance ion source plasmas
title_full Model of charge-state distributions for electron cyclotron resonance ion source plasmas
title_fullStr Model of charge-state distributions for electron cyclotron resonance ion source plasmas
title_full_unstemmed Model of charge-state distributions for electron cyclotron resonance ion source plasmas
title_sort model of charge-state distributions for electron cyclotron resonance ion source plasmas
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 1999-12-01
description A computer model for the ion charge-state distribution (CSD) in an electron cyclotron resonance ion source (ECRIS) plasma is presented that incorporates non-Maxwellian distribution functions, multiple atomic species, and ion confinement due to the ambipolar potential well that arises from confinement of the electron cyclotron resonance (ECR) heated electrons. Atomic processes incorporated into the model include multiple ionization and multiple charge exchange with rate coefficients calculated for non-Maxwellian electron distributions. The electron distribution function is calculated using a Fokker-Planck code with an ECR heating term. This eliminates the electron temperature as an arbitrary user input. The model produces results that are a good match to CSD data from the ANL-ECRII ECRIS. Extending the model to 1D axial will also allow the model to determine the plasma and electrostatic potential profiles, further eliminating arbitrary user input to the model.
url http://doi.org/10.1103/PhysRevSTAB.2.123502
work_keys_str_mv AT dhedgell modelofchargestatedistributionsforelectroncyclotronresonanceionsourceplasmas
AT jskim modelofchargestatedistributionsforelectroncyclotronresonanceionsourceplasmas
AT skwong modelofchargestatedistributionsforelectroncyclotronresonanceionsourceplasmas
AT rcpardo modelofchargestatedistributionsforelectroncyclotronresonanceionsourceplasmas
AT rvondrasek modelofchargestatedistributionsforelectroncyclotronresonanceionsourceplasmas
_version_ 1725979392935460864