Cargando…

The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source

The efficiency of the microwave-plasma coupling plays a significant role in the production of highly charged ion beams with electron cyclotron resonance ion sources (ECRISs). The coupling properties are affected by the mechanical design of the ion source plasma chamber and microwave launching system...

Descripción completa

Detalles Bibliográficos
Autores principales: Tarvainen, O, Orpana, J, Kronholm, R, Kalvas, T, Laulainen, J, Koivisto, H, Izotov, I, Skalyga, V, Toivanen, V
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1063/1.4962026
http://cds.cern.ch/record/2268225
_version_ 1780954708032094208
author Tarvainen, O
Orpana, J
Kronholm, R
Kalvas, T
Laulainen, J
Koivisto, H
Izotov, I
Skalyga, V
Toivanen, V
author_facet Tarvainen, O
Orpana, J
Kronholm, R
Kalvas, T
Laulainen, J
Koivisto, H
Izotov, I
Skalyga, V
Toivanen, V
author_sort Tarvainen, O
collection CERN
description The efficiency of the microwave-plasma coupling plays a significant role in the production of highly charged ion beams with electron cyclotron resonance ion sources (ECRISs). The coupling properties are affected by the mechanical design of the ion source plasma chamber and microwave launching system, as well as damping of the microwave electric field by the plasma. Several experiments attempting to optimize the microwave-plasma coupling characteristics by fine-tuning the frequency of the injected microwaves have been conducted with varying degrees of success. The inherent difficulty in interpretation of the frequency tuning results is that the effects of microwave coupling system and the cavity behavior of the plasma chamber cannot be separated. A preferable approach to study the effect of the cavity properties of the plasma chamber on extracted beam currents is to adjust the cavity dimensions. The results of such cavity tuning experiments conducted with the JYFL 14 GHz ECRIS are reported here. The cavity properties were adjusted by inserting a conducting tuner rod axially into the plasma chamber. The extracted beam currents of oxygen charge states O3+–O7+ were recorded at various tuner positions and frequencies in the range of 14.00–14.15 GHz. It was observed that the tuner position affects the beam currents of high charge state ions up to several tens of percent. In particular, it was found that at some tuner position / frequency combinations the plasma exhibited “mode-hopping” between two operating regimes. The results improve the understanding of the role of plasma chamber cavity properties on ECRIS performances.
id oai-inspirehep.net-1602721
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling oai-inspirehep.net-16027212019-09-30T06:29:59Zdoi:10.1063/1.4962026http://cds.cern.ch/record/2268225engTarvainen, OOrpana, JKronholm, RKalvas, TLaulainen, JKoivisto, HIzotov, ISkalyga, VToivanen, VThe effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion sourceAccelerators and Storage RingsThe efficiency of the microwave-plasma coupling plays a significant role in the production of highly charged ion beams with electron cyclotron resonance ion sources (ECRISs). The coupling properties are affected by the mechanical design of the ion source plasma chamber and microwave launching system, as well as damping of the microwave electric field by the plasma. Several experiments attempting to optimize the microwave-plasma coupling characteristics by fine-tuning the frequency of the injected microwaves have been conducted with varying degrees of success. The inherent difficulty in interpretation of the frequency tuning results is that the effects of microwave coupling system and the cavity behavior of the plasma chamber cannot be separated. A preferable approach to study the effect of the cavity properties of the plasma chamber on extracted beam currents is to adjust the cavity dimensions. The results of such cavity tuning experiments conducted with the JYFL 14 GHz ECRIS are reported here. The cavity properties were adjusted by inserting a conducting tuner rod axially into the plasma chamber. The extracted beam currents of oxygen charge states O3+–O7+ were recorded at various tuner positions and frequencies in the range of 14.00–14.15 GHz. It was observed that the tuner position affects the beam currents of high charge state ions up to several tens of percent. In particular, it was found that at some tuner position / frequency combinations the plasma exhibited “mode-hopping” between two operating regimes. The results improve the understanding of the role of plasma chamber cavity properties on ECRIS performances.oai:inspirehep.net:16027212016
spellingShingle Accelerators and Storage Rings
Tarvainen, O
Orpana, J
Kronholm, R
Kalvas, T
Laulainen, J
Koivisto, H
Izotov, I
Skalyga, V
Toivanen, V
The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source
title The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source
title_full The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source
title_fullStr The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source
title_full_unstemmed The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source
title_short The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source
title_sort effect of cavity tuning on oxygen beam currents of an a-ecr type 14 ghz electron cyclotron resonance ion source
topic Accelerators and Storage Rings
url https://dx.doi.org/10.1063/1.4962026
http://cds.cern.ch/record/2268225
work_keys_str_mv AT tarvaineno theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT orpanaj theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT kronholmr theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT kalvast theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT laulainenj theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT koivistoh theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT izotovi theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT skalygav theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT toivanenv theeffectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT tarvaineno effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT orpanaj effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT kronholmr effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT kalvast effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT laulainenj effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT koivistoh effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT izotovi effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT skalygav effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource
AT toivanenv effectofcavitytuningonoxygenbeamcurrentsofanaecrtype14ghzelectroncyclotronresonanceionsource