{"title":"两级自由电子激光器的腔体设计","authors":"S. von Laven, S. Segall, J. Ward","doi":"10.1109/IRMM.1983.9126530","DOIUrl":null,"url":null,"abstract":"In the KMS Fusion two-stage free electron laser (FEL) experiment, the first-stage and second-stage radiation must suffer low losses in the oscillator. The electromagnetic modes overlap each other (and the electron beam) in a TE01 waveguide but separate before reaching the end mirrors.","PeriodicalId":314918,"journal":{"name":"1983 Eighth International Conference on Infrared and Millimeter Waves","volume":"6 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1983-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Cavity design for a two-stage FEL\",\"authors\":\"S. von Laven, S. Segall, J. Ward\",\"doi\":\"10.1109/IRMM.1983.9126530\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In the KMS Fusion two-stage free electron laser (FEL) experiment, the first-stage and second-stage radiation must suffer low losses in the oscillator. The electromagnetic modes overlap each other (and the electron beam) in a TE01 waveguide but separate before reaching the end mirrors.\",\"PeriodicalId\":314918,\"journal\":{\"name\":\"1983 Eighth International Conference on Infrared and Millimeter Waves\",\"volume\":\"6 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1983-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1983 Eighth International Conference on Infrared and Millimeter Waves\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/IRMM.1983.9126530\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1983 Eighth International Conference on Infrared and Millimeter Waves","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IRMM.1983.9126530","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
In the KMS Fusion two-stage free electron laser (FEL) experiment, the first-stage and second-stage radiation must suffer low losses in the oscillator. The electromagnetic modes overlap each other (and the electron beam) in a TE01 waveguide but separate before reaching the end mirrors.
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