{"title":"各向同性探测器的蚀刻轨迹动力学","authors":"A. Ali , S.A. Durrani","doi":"10.1016/0145-224X(77)90004-7","DOIUrl":null,"url":null,"abstract":"<div><p>As the etching of a charged-particle track proceeds in a detector, three successive phases can be recognized: the “cone phase”, the “transirion phase”, and the “sphere phase”. Equations are derived to give the values of various useful etch-pit parameters, in particular those connected with the surface openings in the three phases. These values are of use in reconstructing the kinematics of the ionizing particle, such as its charge, mass, energy, and range.</p></div>","PeriodicalId":100974,"journal":{"name":"Nuclear Track Detection","volume":"1 2","pages":"Pages 107-121"},"PeriodicalIF":0.0000,"publicationDate":"1977-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0145-224X(77)90004-7","citationCount":"19","resultStr":"{\"title\":\"Etched-track kinetics in isotropic detectors\",\"authors\":\"A. Ali , S.A. Durrani\",\"doi\":\"10.1016/0145-224X(77)90004-7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>As the etching of a charged-particle track proceeds in a detector, three successive phases can be recognized: the “cone phase”, the “transirion phase”, and the “sphere phase”. Equations are derived to give the values of various useful etch-pit parameters, in particular those connected with the surface openings in the three phases. These values are of use in reconstructing the kinematics of the ionizing particle, such as its charge, mass, energy, and range.</p></div>\",\"PeriodicalId\":100974,\"journal\":{\"name\":\"Nuclear Track Detection\",\"volume\":\"1 2\",\"pages\":\"Pages 107-121\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1977-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0145-224X(77)90004-7\",\"citationCount\":\"19\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Track Detection\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0145224X77900047\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Track Detection","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0145224X77900047","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
As the etching of a charged-particle track proceeds in a detector, three successive phases can be recognized: the “cone phase”, the “transirion phase”, and the “sphere phase”. Equations are derived to give the values of various useful etch-pit parameters, in particular those connected with the surface openings in the three phases. These values are of use in reconstructing the kinematics of the ionizing particle, such as its charge, mass, energy, and range.