A. Berezin, Y. Faǐnberg, G. Berezina, L. I. Bolotin, V. G. Stupak
{"title":"强电子束与等离子体的相互作用","authors":"A. Berezin, Y. Faǐnberg, G. Berezina, L. I. Bolotin, V. G. Stupak","doi":"10.1088/0368-3281/4/4/308","DOIUrl":null,"url":null,"abstract":"The energy losses of an originally unmodulated electron beam during its passage through a plasma which is not in a magnetic field have been determined experimentally. With a current of 8 A, an energy of 26 keV and a plasma density of (-7 similar 9) × 1010 cm-3, these losses amount to 12 per cent of the energy of the electron beam. It is shown that these large energy losses are due to the coherent interaction of the beam with the plasma.","PeriodicalId":8612,"journal":{"name":"atomnaya Energ","volume":"8 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"1961-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":"{\"title\":\"INTERACTION OF STRONG ELECTRON BEAMS WITH PLASMA\",\"authors\":\"A. Berezin, Y. Faǐnberg, G. Berezina, L. I. Bolotin, V. G. Stupak\",\"doi\":\"10.1088/0368-3281/4/4/308\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The energy losses of an originally unmodulated electron beam during its passage through a plasma which is not in a magnetic field have been determined experimentally. With a current of 8 A, an energy of 26 keV and a plasma density of (-7 similar 9) × 1010 cm-3, these losses amount to 12 per cent of the energy of the electron beam. It is shown that these large energy losses are due to the coherent interaction of the beam with the plasma.\",\"PeriodicalId\":8612,\"journal\":{\"name\":\"atomnaya Energ\",\"volume\":\"8 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1961-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"5\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"atomnaya Energ\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/0368-3281/4/4/308\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"atomnaya Energ","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0368-3281/4/4/308","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The energy losses of an originally unmodulated electron beam during its passage through a plasma which is not in a magnetic field have been determined experimentally. With a current of 8 A, an energy of 26 keV and a plasma density of (-7 similar 9) × 1010 cm-3, these losses amount to 12 per cent of the energy of the electron beam. It is shown that these large energy losses are due to the coherent interaction of the beam with the plasma.
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