{"title":"Quantitative autoradiographic measurement of the scattering of protons in a krypton gas target","authors":"J.J.L. Mulders, L.W.G. Steenhuysen","doi":"10.1016/0020-708X(85)90015-8","DOIUrl":null,"url":null,"abstract":"<div><p>A study on the measurements of proton current density profiles determined by the scattering process in natural krypton gas resulted in the development of a quantitative autoradiographic technique for the determination of a proton induced activity distribution on a Cu foil. Application of this technique showed that a 24 MeV, 1 μA proton beam with a FWHM of 7.3 mm was enlarged to a beam with a FWHM of about 43.5 mm for a target length of 50 cm and a Kr gas pressure of 400 kPa. For a comparison the target was also filled with Xe gas resulting in a larger FWHM value than for krypton under the same experimental conditions.</p></div>","PeriodicalId":22517,"journal":{"name":"The International journal of applied radiation and isotopes","volume":"36 11","pages":"Pages 833-841"},"PeriodicalIF":0.0000,"publicationDate":"1985-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0020-708X(85)90015-8","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The International journal of applied radiation and isotopes","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0020708X85900158","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
A study on the measurements of proton current density profiles determined by the scattering process in natural krypton gas resulted in the development of a quantitative autoradiographic technique for the determination of a proton induced activity distribution on a Cu foil. Application of this technique showed that a 24 MeV, 1 μA proton beam with a FWHM of 7.3 mm was enlarged to a beam with a FWHM of about 43.5 mm for a target length of 50 cm and a Kr gas pressure of 400 kPa. For a comparison the target was also filled with Xe gas resulting in a larger FWHM value than for krypton under the same experimental conditions.