{"title":"带光子辐射的电子-正电子对的非共振光产生","authors":"P. Fomin, R. Kholodov","doi":"10.1109/LFNM.2010.5624164","DOIUrl":null,"url":null,"abstract":"The process of photon emission, that accompany photon pair production in strong magnetic field has been studied in nonresonant case. Angle dependence and dependence on final photon polarization are analyzed for this process. Total probability for the nonresonant process of photon emission 106 s−1 is three order of magnitude less, than resonant one. PACS: 12.20.-m; 41.60. Ap; 42.25. Ja","PeriodicalId":117420,"journal":{"name":"2010 10th International Conference on Laser and Fiber-Optical Networks Modeling","volume":"1172 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2010-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Nonresonant photoproduction of an electron-positron pair with radiation of a photon\",\"authors\":\"P. Fomin, R. Kholodov\",\"doi\":\"10.1109/LFNM.2010.5624164\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The process of photon emission, that accompany photon pair production in strong magnetic field has been studied in nonresonant case. Angle dependence and dependence on final photon polarization are analyzed for this process. Total probability for the nonresonant process of photon emission 106 s−1 is three order of magnitude less, than resonant one. PACS: 12.20.-m; 41.60. Ap; 42.25. Ja\",\"PeriodicalId\":117420,\"journal\":{\"name\":\"2010 10th International Conference on Laser and Fiber-Optical Networks Modeling\",\"volume\":\"1172 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2010-11-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2010 10th International Conference on Laser and Fiber-Optical Networks Modeling\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/LFNM.2010.5624164\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2010 10th International Conference on Laser and Fiber-Optical Networks Modeling","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/LFNM.2010.5624164","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Nonresonant photoproduction of an electron-positron pair with radiation of a photon
The process of photon emission, that accompany photon pair production in strong magnetic field has been studied in nonresonant case. Angle dependence and dependence on final photon polarization are analyzed for this process. Total probability for the nonresonant process of photon emission 106 s−1 is three order of magnitude less, than resonant one. PACS: 12.20.-m; 41.60. Ap; 42.25. Ja
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