{"title":"Fourier transform mass spectrometry in an ECR plasma","authors":"J. Shohet, J. Friedmann, A. Wendt, J. Brenna","doi":"10.1109/PLASMA.1989.166244","DOIUrl":null,"url":null,"abstract":"Consideration has been given to the use of Fourier transform mass spectrometry (FTMS) to provide in-situ mass measurements of active species in an electron cyclotron resonance (ECR) plasma reactor. An ECR plasma was produced in a vacuum chamber placed inside a DC magnetic mirror field by microwaves whose power level could be adjusted up to 2 kW CW. The electron cyclotron resonance was adjusted to be approximately 25% of the distance from the throat of the mirror to the mid-plane of the vacuum chamber. The mirror ratio was 2:1, the operating gas was argon, and the pressure was set to 2*10/sup -4/ torr. FTMS took place in a cubical cell placed in the center of the magnetic mirror region where the magnetic field was most uniform.<<ETX>>","PeriodicalId":165717,"journal":{"name":"IEEE 1989 International Conference on Plasma Science","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1989-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE 1989 International Conference on Plasma Science","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PLASMA.1989.166244","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
Consideration has been given to the use of Fourier transform mass spectrometry (FTMS) to provide in-situ mass measurements of active species in an electron cyclotron resonance (ECR) plasma reactor. An ECR plasma was produced in a vacuum chamber placed inside a DC magnetic mirror field by microwaves whose power level could be adjusted up to 2 kW CW. The electron cyclotron resonance was adjusted to be approximately 25% of the distance from the throat of the mirror to the mid-plane of the vacuum chamber. The mirror ratio was 2:1, the operating gas was argon, and the pressure was set to 2*10/sup -4/ torr. FTMS took place in a cubical cell placed in the center of the magnetic mirror region where the magnetic field was most uniform.<>