{"title":"Optimal Targeting of a Tumor through Proton Beam Therapy","authors":"K. Pant, C. Campbell","doi":"10.22186/jyi.37.3.32-37","DOIUrl":null,"url":null,"abstract":"Publication date: March 2020 the prostate, esophagus, lung and liver. A large number of pediatric patients with central nervous system (CNS) tumors also benefit from PBT (Gondi et al., 2016). Protons interact with matter in three different ways: interactions with atomic electrons, interactions with the atomic nucleus, and interactions with the atom as a whole (Verhey et al., 1998). Protons that interact with the nucleus may produce Bremsstrahlung radiation, but this occurs so infrequently that its effects are negligible. There is also the possibility that protons will collide with an atom and produce secondary protons, neutrons, or excited nuclei, although these interactions are also rare. Protons primarily lose kinetic energy as they traverse matter via inelastic Coulombic interactions with atomic orbital electrons, which also deflect the proton trajectory (Newhauser and Zhang, 2015). The deflection due to a single interaction is generally quite small as the mass of a proton is much larger than that of an electron. However, the cumulative effect of many such interactions can be significant. The most complete theory of multiple Coulombic scattering was proposed by Molière (1947). Many simplifications of this theory have been proposed, although this simplicity often reduces the accuracy in modeling Coulombic scattering at large angles. Gottschalk et al. (1993) approximated Molière’s theory to take the form of a Gaussian function, assuming the small angle approximation in which sin(θ)≈θ:","PeriodicalId":74021,"journal":{"name":"Journal of young investigators","volume":"37 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2020-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of young investigators","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.22186/jyi.37.3.32-37","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Publication date: March 2020 the prostate, esophagus, lung and liver. A large number of pediatric patients with central nervous system (CNS) tumors also benefit from PBT (Gondi et al., 2016). Protons interact with matter in three different ways: interactions with atomic electrons, interactions with the atomic nucleus, and interactions with the atom as a whole (Verhey et al., 1998). Protons that interact with the nucleus may produce Bremsstrahlung radiation, but this occurs so infrequently that its effects are negligible. There is also the possibility that protons will collide with an atom and produce secondary protons, neutrons, or excited nuclei, although these interactions are also rare. Protons primarily lose kinetic energy as they traverse matter via inelastic Coulombic interactions with atomic orbital electrons, which also deflect the proton trajectory (Newhauser and Zhang, 2015). The deflection due to a single interaction is generally quite small as the mass of a proton is much larger than that of an electron. However, the cumulative effect of many such interactions can be significant. The most complete theory of multiple Coulombic scattering was proposed by Molière (1947). Many simplifications of this theory have been proposed, although this simplicity often reduces the accuracy in modeling Coulombic scattering at large angles. Gottschalk et al. (1993) approximated Molière’s theory to take the form of a Gaussian function, assuming the small angle approximation in which sin(θ)≈θ:
出版日期:2020年3月前列腺、食道、肺和肝。大量患有中枢神经系统(CNS)肿瘤的儿科患者也受益于PBT (Gondi et al., 2016)。质子以三种不同的方式与物质相互作用:与原子电子的相互作用,与原子核的相互作用,以及与整个原子的相互作用(Verhey et al., 1998)。质子与原子核相互作用可能产生轫致辐射,但这种情况很少发生,其影响可以忽略不计。也有可能质子与原子碰撞并产生二次质子、中子或激发态原子核,尽管这些相互作用也很罕见。质子通过与原子轨道电子的非弹性库仑相互作用穿越物质时主要失去动能,这也会使质子轨迹偏斜(Newhauser和Zhang, 2015)。由于质子的质量比电子的质量大得多,单次相互作用引起的偏转通常相当小。然而,许多这样的相互作用的累积效应可能是显著的。最完整的多重库仑散射理论是由moli(1947)提出的。人们对这一理论进行了许多简化,尽管这种简化往往会降低大角度库仑散射建模的准确性。Gottschalk et al.(1993)将moli的理论近似为高斯函数的形式,假设sin(θ)≈θ的小角度近似: