{"title":"八次谐波cuscusron管的实验","authors":"K. Tiong, S. Kuo, P. E. Miller","doi":"10.1109/irmm.1987.9127085","DOIUrl":null,"url":null,"abstract":"We have set up a cusptron device to compare the performance of π mode and 2π mode operation at 8th harmonic interaction. A concentric e-layer of of 30 Kev (γ=1.06) is produced for wave generation. For 2π mode operation, an 8-slotted waveguide with b/a = 22 is used, where b and a are the radii of the vane and the inner wall of the waveguide respectively. In order to achieve same output frequency for comparison, a 16-slotted waveguide with b/a =1.23 is used for π mode operation. The arrangement of the set up will be described. The preliminary results of the experiments will also be presented.","PeriodicalId":399243,"journal":{"name":"1987 Twelth International Conference on Infrared and Millimeter Waves","volume":"14 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1987-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Experiments for an eighth harmonic cusptron tube\",\"authors\":\"K. Tiong, S. Kuo, P. E. Miller\",\"doi\":\"10.1109/irmm.1987.9127085\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We have set up a cusptron device to compare the performance of π mode and 2π mode operation at 8th harmonic interaction. A concentric e-layer of of 30 Kev (γ=1.06) is produced for wave generation. For 2π mode operation, an 8-slotted waveguide with b/a = 22 is used, where b and a are the radii of the vane and the inner wall of the waveguide respectively. In order to achieve same output frequency for comparison, a 16-slotted waveguide with b/a =1.23 is used for π mode operation. The arrangement of the set up will be described. The preliminary results of the experiments will also be presented.\",\"PeriodicalId\":399243,\"journal\":{\"name\":\"1987 Twelth International Conference on Infrared and Millimeter Waves\",\"volume\":\"14 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1987-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1987 Twelth International Conference on Infrared and Millimeter Waves\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/irmm.1987.9127085\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1987 Twelth International Conference on Infrared and Millimeter Waves","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/irmm.1987.9127085","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
We have set up a cusptron device to compare the performance of π mode and 2π mode operation at 8th harmonic interaction. A concentric e-layer of of 30 Kev (γ=1.06) is produced for wave generation. For 2π mode operation, an 8-slotted waveguide with b/a = 22 is used, where b and a are the radii of the vane and the inner wall of the waveguide respectively. In order to achieve same output frequency for comparison, a 16-slotted waveguide with b/a =1.23 is used for π mode operation. The arrangement of the set up will be described. The preliminary results of the experiments will also be presented.
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