{"title":"A Linac-Driven XUV Free-Electron Laser","authors":"B. Newnam, J. Goldstein, J. Fraser, R. Cooper","doi":"10.1063/1.34635","DOIUrl":null,"url":null,"abstract":"An XUV free-electron laser (FEL) driven by a linear accelerator appears to be feasible for wavelengths as short as 50 nm. This projection is based upon the anticipated successful use of high peak-current (~100 A) linacs in forthcoming FEL oscillator experiments at infrared and visible wavelengths at Los Alamos and Boeing/Mathematical Sciences Northwest. As an alternative to schemes involving storage rings, a linac provides a train of individual electron bunches separated by 10-100 ns and duration of 10-30 ps. Further, electrons pass through the undulator magnet only once, but their remaining energy may be recovered in a separate decelerating structure and fed back into the primary accelerator.","PeriodicalId":436319,"journal":{"name":"Topical Meeting on Free Electron Generation of Extreme Ultraviolet Coherent Radiation","volume":"31 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1984-06-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"8","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Topical Meeting on Free Electron Generation of Extreme Ultraviolet Coherent Radiation","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.34635","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 8
Abstract
An XUV free-electron laser (FEL) driven by a linear accelerator appears to be feasible for wavelengths as short as 50 nm. This projection is based upon the anticipated successful use of high peak-current (~100 A) linacs in forthcoming FEL oscillator experiments at infrared and visible wavelengths at Los Alamos and Boeing/Mathematical Sciences Northwest. As an alternative to schemes involving storage rings, a linac provides a train of individual electron bunches separated by 10-100 ns and duration of 10-30 ps. Further, electrons pass through the undulator magnet only once, but their remaining energy may be recovered in a separate decelerating structure and fed back into the primary accelerator.