{"title":"PPM系统中的电子束传播","authors":"E. A. Périgo, R. Faria, J. Barroso, C. Motta","doi":"10.1109/PPC.2005.300629","DOIUrl":null,"url":null,"abstract":"By using a 2.5 and 3-D particle-in-cell code, this paper reports on the electron beam propagation behavior, in a drift tube, under different acceleration potentials ranging from 15 kV to 125 kV in a PPM (periodic-permanent magnet) focusing structure. The investigation is carried out under two approaches. First, an electron beam with a constant electric current of Iomicron = 24 A is injected into a drift tube. Second, an electron beam with a constant perveance of 0.77 mu Perv is injected in the same drift tube. In both cases, the peak of axial component of the magnetic density flux is Bomicron = 173 mT and the PPM period is L = 24 mm. The analysis is centered on evaluating both the magnetic field parameter a, which determines the theoretical conditions for a satisfactory transmission of the beam through the drift tube and the azimuthal momentum of the electrons.","PeriodicalId":200159,"journal":{"name":"2005 IEEE Pulsed Power Conference","volume":"15 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2005-06-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Electron Beam Propagation in a PPM System\",\"authors\":\"E. A. Périgo, R. Faria, J. Barroso, C. Motta\",\"doi\":\"10.1109/PPC.2005.300629\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"By using a 2.5 and 3-D particle-in-cell code, this paper reports on the electron beam propagation behavior, in a drift tube, under different acceleration potentials ranging from 15 kV to 125 kV in a PPM (periodic-permanent magnet) focusing structure. The investigation is carried out under two approaches. First, an electron beam with a constant electric current of Iomicron = 24 A is injected into a drift tube. Second, an electron beam with a constant perveance of 0.77 mu Perv is injected in the same drift tube. In both cases, the peak of axial component of the magnetic density flux is Bomicron = 173 mT and the PPM period is L = 24 mm. The analysis is centered on evaluating both the magnetic field parameter a, which determines the theoretical conditions for a satisfactory transmission of the beam through the drift tube and the azimuthal momentum of the electrons.\",\"PeriodicalId\":200159,\"journal\":{\"name\":\"2005 IEEE Pulsed Power Conference\",\"volume\":\"15 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2005-06-13\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2005 IEEE Pulsed Power Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PPC.2005.300629\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2005 IEEE Pulsed Power Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PPC.2005.300629","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
By using a 2.5 and 3-D particle-in-cell code, this paper reports on the electron beam propagation behavior, in a drift tube, under different acceleration potentials ranging from 15 kV to 125 kV in a PPM (periodic-permanent magnet) focusing structure. The investigation is carried out under two approaches. First, an electron beam with a constant electric current of Iomicron = 24 A is injected into a drift tube. Second, an electron beam with a constant perveance of 0.77 mu Perv is injected in the same drift tube. In both cases, the peak of axial component of the magnetic density flux is Bomicron = 173 mT and the PPM period is L = 24 mm. The analysis is centered on evaluating both the magnetic field parameter a, which determines the theoretical conditions for a satisfactory transmission of the beam through the drift tube and the azimuthal momentum of the electrons.