{"title":"磁场中使用阿斯穆森腔产生等离子体","authors":"S. D. De Souza-Machado, J. Curry, F. Skiff","doi":"10.1109/PLASMA.1994.589006","DOIUrl":null,"url":null,"abstract":"The density, temperature and flow speed of an argon plasma produced by an Asmussen cavity in a weak magnetic field is measured using Laser Induced Fluorescence and Langmuir probes. The sour is at one end of a main chamber that is in a magnetic mirror configuration, with pancake coils arranged at both the source end and the far end. The magnetic field at the source is below that required for ECR. The 2.45 GHz microwave resonant cavity has a diameter of 10.2 cm, with a 1.8 cm O.D. (1.35 cm I.D.) on-axis quartz tube within which the plasma is created, both of which are smaller than many of the Asmussen cavities described in the current literature.","PeriodicalId":254741,"journal":{"name":"Proceedings of 1994 IEEE 21st International Conference on Plasma Sciences (ICOPS)","volume":"73 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1994-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Plasma Production Using An Asmussen Cavity In A Magnetic Field\",\"authors\":\"S. D. De Souza-Machado, J. Curry, F. Skiff\",\"doi\":\"10.1109/PLASMA.1994.589006\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The density, temperature and flow speed of an argon plasma produced by an Asmussen cavity in a weak magnetic field is measured using Laser Induced Fluorescence and Langmuir probes. The sour is at one end of a main chamber that is in a magnetic mirror configuration, with pancake coils arranged at both the source end and the far end. The magnetic field at the source is below that required for ECR. The 2.45 GHz microwave resonant cavity has a diameter of 10.2 cm, with a 1.8 cm O.D. (1.35 cm I.D.) on-axis quartz tube within which the plasma is created, both of which are smaller than many of the Asmussen cavities described in the current literature.\",\"PeriodicalId\":254741,\"journal\":{\"name\":\"Proceedings of 1994 IEEE 21st International Conference on Plasma Sciences (ICOPS)\",\"volume\":\"73 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1994-06-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of 1994 IEEE 21st International Conference on Plasma Sciences (ICOPS)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PLASMA.1994.589006\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of 1994 IEEE 21st International Conference on Plasma Sciences (ICOPS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PLASMA.1994.589006","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Plasma Production Using An Asmussen Cavity In A Magnetic Field
The density, temperature and flow speed of an argon plasma produced by an Asmussen cavity in a weak magnetic field is measured using Laser Induced Fluorescence and Langmuir probes. The sour is at one end of a main chamber that is in a magnetic mirror configuration, with pancake coils arranged at both the source end and the far end. The magnetic field at the source is below that required for ECR. The 2.45 GHz microwave resonant cavity has a diameter of 10.2 cm, with a 1.8 cm O.D. (1.35 cm I.D.) on-axis quartz tube within which the plasma is created, both of which are smaller than many of the Asmussen cavities described in the current literature.
京公网安备 11010802042870号
京ICP备2023020795号-1
分享
求助内容：
应助结果提醒方式：
扫码关注我们
