{"title":"均匀康普顿散射体中的伽马射线","authors":"V. Uchaikin","doi":"10.15406/paij.2018.02.00144","DOIUrl":null,"url":null,"abstract":"Describing the transport of particles in a medium from a source with phase density ( ) Q x immersed in a medium, interaction of which with the particles is described by the operator L. In the problem under consideration, ( ) f x may denote the flux of photons, or their concentration, or some other local characteristics of the photon field at a point = ( , ) x r p of the phase space. For the sake of convenience, we will represent the photon momentum p through the pair of variables = / p Ω p (the direction unit vector) and = E cp (photon’s energy).","PeriodicalId":137635,"journal":{"name":"Physics & Astronomy International Journal","volume":"5 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-12-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"A Gamma-ray in a uniform compton scatterer\",\"authors\":\"V. Uchaikin\",\"doi\":\"10.15406/paij.2018.02.00144\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Describing the transport of particles in a medium from a source with phase density ( ) Q x immersed in a medium, interaction of which with the particles is described by the operator L. In the problem under consideration, ( ) f x may denote the flux of photons, or their concentration, or some other local characteristics of the photon field at a point = ( , ) x r p of the phase space. For the sake of convenience, we will represent the photon momentum p through the pair of variables = / p Ω p (the direction unit vector) and = E cp (photon’s energy).\",\"PeriodicalId\":137635,\"journal\":{\"name\":\"Physics & Astronomy International Journal\",\"volume\":\"5 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2018-12-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physics & Astronomy International Journal\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.15406/paij.2018.02.00144\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physics & Astronomy International Journal","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.15406/paij.2018.02.00144","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
摘要
描述粒子在介质中的输运,其源的相密度()Q x浸没在介质中,介质与粒子的相互作用用算符l来描述。在考虑的问题中,()f x可以表示光子的通量,或者它们的浓度,或者光子场在相空间点= (,)x r p处的其他一些局部特征。为了方便起见,我们将通过一对变量= / p Ω p(方向单位矢量)和= E cp(光子能量)来表示光子动量p。
Describing the transport of particles in a medium from a source with phase density ( ) Q x immersed in a medium, interaction of which with the particles is described by the operator L. In the problem under consideration, ( ) f x may denote the flux of photons, or their concentration, or some other local characteristics of the photon field at a point = ( , ) x r p of the phase space. For the sake of convenience, we will represent the photon momentum p through the pair of variables = / p Ω p (the direction unit vector) and = E cp (photon’s energy).