{"title":"自由电子激光器的单模效率","authors":"J. Soln","doi":"10.1109/irmm.1983.9126507","DOIUrl":null,"url":null,"abstract":"For free-electron laser (FEL) devices with dilute and cold electron beams, an expression for the single-mode efficiency, ∊, is defined. The connection with the full (quantum mechanical) gain, G, is such that ∊/G is equal to the ratio of the total photon energy to the kinetic electron-beam energy “trapped” in the interaction volume V. Both ∊ and G are discussed quantitatively, using the example of a quantum model of the Smith-Purcell FEL: it is shown that unlike G, ∊ depends on the total photon energy trapped in V even in the classical regime.","PeriodicalId":314918,"journal":{"name":"1983 Eighth International Conference on Infrared and Millimeter Waves","volume":"65 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1983-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Single-mode efficiency in free-electron lasers\",\"authors\":\"J. Soln\",\"doi\":\"10.1109/irmm.1983.9126507\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"For free-electron laser (FEL) devices with dilute and cold electron beams, an expression for the single-mode efficiency, ∊, is defined. The connection with the full (quantum mechanical) gain, G, is such that ∊/G is equal to the ratio of the total photon energy to the kinetic electron-beam energy “trapped” in the interaction volume V. Both ∊ and G are discussed quantitatively, using the example of a quantum model of the Smith-Purcell FEL: it is shown that unlike G, ∊ depends on the total photon energy trapped in V even in the classical regime.\",\"PeriodicalId\":314918,\"journal\":{\"name\":\"1983 Eighth International Conference on Infrared and Millimeter Waves\",\"volume\":\"65 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.1983.9126507\",\"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.1983.9126507","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
For free-electron laser (FEL) devices with dilute and cold electron beams, an expression for the single-mode efficiency, ∊, is defined. The connection with the full (quantum mechanical) gain, G, is such that ∊/G is equal to the ratio of the total photon energy to the kinetic electron-beam energy “trapped” in the interaction volume V. Both ∊ and G are discussed quantitatively, using the example of a quantum model of the Smith-Purcell FEL: it is shown that unlike G, ∊ depends on the total photon energy trapped in V even in the classical regime.