C. Leroy, P. Roy, G. Casse, M. Glaser, E. Grigoriev, F. Lemeilleur
{"title":"未辐照和辐照硅二极管中的电荷输运","authors":"C. Leroy, P. Roy, G. Casse, M. Glaser, E. Grigoriev, F. Lemeilleur","doi":"10.1109/NSSMIC.1998.775147","DOIUrl":null,"url":null,"abstract":"A model describing the transport of charge carriers generated in silicon detectors (standard planar float zone and MESA diodes) by ionizing particles is presented. The current pulse response induced by /spl alpha/ and /spl beta/ particles in non-irradiated detectors and detectors irradiated up to fluences /spl Phi//spl ap/3/spl middot/10/sup 14/ particles/cm/sup 2/ is reproduced through this model: i) by adding a small n-type region 15 /spl mu/m deep on the p/sup +/ side for the standard planar float zone detectors at fluences beyond the n to p-type inversion and ii) for the MESA detectors, by considering one dead layer 14 /spl mu/m deep (observed experimentally) on each side, and introducing a second (delayed) component. For both types of detectors, the model gives mobilities decreasing linearity up to fluences of about 5/spl middot/10/sup 13/ particles/cm/sup 2/ and converging, beyond, to saturation values of about 1000 cm/sup 2//Vs and 455 cm/sup 2//Vs for electrons and holes, respectively. At a fluence /spl Phi//spl ap/10/sup 14/ particles/cm/sup 2/, charge collection deficits of about 13% for /spl beta/ particles, 25% for /spl alpha/ particles incident on the front and 35% for /spl alpha/ particles incident on the back of the detector are found for both type of diodes.","PeriodicalId":129202,"journal":{"name":"1998 IEEE Nuclear Science Symposium Conference Record. 1998 IEEE Nuclear Science Symposium and Medical Imaging Conference (Cat. No.98CH36255)","volume":"114 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-11-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Charge transport in non-irradiated and irradiated silicon diodes\",\"authors\":\"C. Leroy, P. Roy, G. Casse, M. Glaser, E. Grigoriev, F. Lemeilleur\",\"doi\":\"10.1109/NSSMIC.1998.775147\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A model describing the transport of charge carriers generated in silicon detectors (standard planar float zone and MESA diodes) by ionizing particles is presented. The current pulse response induced by /spl alpha/ and /spl beta/ particles in non-irradiated detectors and detectors irradiated up to fluences /spl Phi//spl ap/3/spl middot/10/sup 14/ particles/cm/sup 2/ is reproduced through this model: i) by adding a small n-type region 15 /spl mu/m deep on the p/sup +/ side for the standard planar float zone detectors at fluences beyond the n to p-type inversion and ii) for the MESA detectors, by considering one dead layer 14 /spl mu/m deep (observed experimentally) on each side, and introducing a second (delayed) component. For both types of detectors, the model gives mobilities decreasing linearity up to fluences of about 5/spl middot/10/sup 13/ particles/cm/sup 2/ and converging, beyond, to saturation values of about 1000 cm/sup 2//Vs and 455 cm/sup 2//Vs for electrons and holes, respectively. At a fluence /spl Phi//spl ap/10/sup 14/ particles/cm/sup 2/, charge collection deficits of about 13% for /spl beta/ particles, 25% for /spl alpha/ particles incident on the front and 35% for /spl alpha/ particles incident on the back of the detector are found for both type of diodes.\",\"PeriodicalId\":129202,\"journal\":{\"name\":\"1998 IEEE Nuclear Science Symposium Conference Record. 1998 IEEE Nuclear Science Symposium and Medical Imaging Conference (Cat. No.98CH36255)\",\"volume\":\"114 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1998-11-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1998 IEEE Nuclear Science Symposium Conference Record. 1998 IEEE Nuclear Science Symposium and Medical Imaging Conference (Cat. No.98CH36255)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/NSSMIC.1998.775147\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1998 IEEE Nuclear Science Symposium Conference Record. 1998 IEEE Nuclear Science Symposium and Medical Imaging Conference (Cat. No.98CH36255)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NSSMIC.1998.775147","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Charge transport in non-irradiated and irradiated silicon diodes
A model describing the transport of charge carriers generated in silicon detectors (standard planar float zone and MESA diodes) by ionizing particles is presented. The current pulse response induced by /spl alpha/ and /spl beta/ particles in non-irradiated detectors and detectors irradiated up to fluences /spl Phi//spl ap/3/spl middot/10/sup 14/ particles/cm/sup 2/ is reproduced through this model: i) by adding a small n-type region 15 /spl mu/m deep on the p/sup +/ side for the standard planar float zone detectors at fluences beyond the n to p-type inversion and ii) for the MESA detectors, by considering one dead layer 14 /spl mu/m deep (observed experimentally) on each side, and introducing a second (delayed) component. For both types of detectors, the model gives mobilities decreasing linearity up to fluences of about 5/spl middot/10/sup 13/ particles/cm/sup 2/ and converging, beyond, to saturation values of about 1000 cm/sup 2//Vs and 455 cm/sup 2//Vs for electrons and holes, respectively. At a fluence /spl Phi//spl ap/10/sup 14/ particles/cm/sup 2/, charge collection deficits of about 13% for /spl beta/ particles, 25% for /spl alpha/ particles incident on the front and 35% for /spl alpha/ particles incident on the back of the detector are found for both type of diodes.