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dc.contributor.authorLuntinen, M.
dc.contributor.authorToivanen, V.
dc.contributor.authorKoivisto, H.
dc.contributor.authorAngot, J.
dc.contributor.authorThuillier, T.
dc.contributor.authorTarvainen, O.
dc.contributor.authorCastro, G.
dc.date.accessioned2023-01-03T09:29:24Z
dc.date.available2023-01-03T09:29:24Z
dc.date.issued2022
dc.identifier.citationLuntinen, M., Toivanen, V., Koivisto, H., Angot, J., Thuillier, T., Tarvainen, O., & Castro, G. (2022). Diagnostics of highly charged plasmas with multicomponent 1+ ion injection. <i>Physical Review E</i>, <i>106</i>(5), Article 055208. <a href="https://doi.org/10.1103/PhysRevE.106.055208" target="_blank">https://doi.org/10.1103/PhysRevE.106.055208</a>
dc.identifier.otherCONVID_164832520
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/84704
dc.description.abstractWe establish multicomponent 1+ injection into a charge breeder electron cyclotron resonance ion source and an associated computational procedure as a noninvasive probe of the electron density ne, average electron energy ⟨Ee⟩, and the characteristic times of ionization, charge exchange, and ion confinement of stochastically heated, highly charged plasma. Multicomponent injection allows refining the ne, ⟨Ee⟩ ranges, reducing experimental uncertainty. Na/K injection is presented as a demonstration. The ⟨Ee⟩ and ne of a hydrogen discharge are found to be 600+600−300eV and 8+8−3×1011cm−3, respectively. The ionization, charge exchange, and confinement times of high charge state alkali ions are on the order of 1 ms–10 ms.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review E
dc.rightsIn Copyright
dc.titleDiagnostics of highly charged plasmas with multicomponent 1+ ion injection
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202301031061
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineKiihdytinlaboratoriofi
dc.contributor.oppiaineAccelerator Laboratoryen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2470-0045
dc.relation.numberinseries5
dc.relation.volume106
dc.type.versionpublishedVersion
dc.rights.copyright©2022 American Physical Society
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber315855
dc.subject.ysoenergia
dc.subject.ysofysiikka
dc.subject.ysoionit
dc.subject.ysomittausmenetelmät
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p1310
jyx.subject.urihttp://www.yso.fi/onto/yso/p900
jyx.subject.urihttp://www.yso.fi/onto/yso/p9015
jyx.subject.urihttp://www.yso.fi/onto/yso/p20083
dc.rights.urlhttp://rightsstatements.org/page/InC/1.0/?language=en
dc.relation.doi10.1103/PhysRevE.106.055208
dc.relation.funderResearch Council of Finlanden
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundinginformationWe acknowledge grants of computer capacity from the Finnish Grid and Cloud Infrastructure [39] and support of the Academy of Finland Project funding (Grant No. 315855).
dc.type.okmA1


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