L. Jastrzebski, R. Duru, D. Le-Cunff, M. Cannac, S. Joblot, I. Mica, M. Polignano, A. Galbiati, P. Monge, Roffarello, G. Nadudvari, Z. Kiss, I. Lajtos, A. Pongrácz, G. Molnár, M. Nagy, L. Dudás, P. Basa, B. Greenwood, J. Gambino
{"title":"缺陷光致发光成像(DPLI)在集成电路加工中的应用综述","authors":"L. Jastrzebski, R. Duru, D. Le-Cunff, M. Cannac, S. Joblot, I. Mica, M. Polignano, A. Galbiati, P. Monge, Roffarello, G. Nadudvari, Z. Kiss, I. Lajtos, A. Pongrácz, G. Molnár, M. Nagy, L. Dudás, P. Basa, B. Greenwood, J. Gambino","doi":"10.23919/IWJT.2019.8802893","DOIUrl":null,"url":null,"abstract":"As Si is an indirect band gap material, the PL generated by phonon assisted band-to-band (B2B) radiative recombination (of energy equal to energy gap of Si) is very weak; about 10 orders of magnitude lower than the exciting photon flux [1] . If crystallographic defects are present then at room temperature an additional broad defect PL peak is generated (DPL) with energy smaller than the band gap of Si [1] , [2] , [3] . At room temperature, defect-band PL intensity is orders of magnitude lower than the B2B intensity [1] .","PeriodicalId":441279,"journal":{"name":"2019 19th International Workshop on Junction Technology (IWJT)","volume":"64 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Review of applications of Defect Photoluminescence Imaging (DPLI) during IC processing\",\"authors\":\"L. Jastrzebski, R. Duru, D. Le-Cunff, M. Cannac, S. Joblot, I. Mica, M. Polignano, A. Galbiati, P. Monge, Roffarello, G. Nadudvari, Z. Kiss, I. Lajtos, A. Pongrácz, G. Molnár, M. Nagy, L. Dudás, P. Basa, B. Greenwood, J. Gambino\",\"doi\":\"10.23919/IWJT.2019.8802893\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"As Si is an indirect band gap material, the PL generated by phonon assisted band-to-band (B2B) radiative recombination (of energy equal to energy gap of Si) is very weak; about 10 orders of magnitude lower than the exciting photon flux [1] . If crystallographic defects are present then at room temperature an additional broad defect PL peak is generated (DPL) with energy smaller than the band gap of Si [1] , [2] , [3] . At room temperature, defect-band PL intensity is orders of magnitude lower than the B2B intensity [1] .\",\"PeriodicalId\":441279,\"journal\":{\"name\":\"2019 19th International Workshop on Junction Technology (IWJT)\",\"volume\":\"64 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-06-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2019 19th International Workshop on Junction Technology (IWJT)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.23919/IWJT.2019.8802893\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 19th International Workshop on Junction Technology (IWJT)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.23919/IWJT.2019.8802893","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Review of applications of Defect Photoluminescence Imaging (DPLI) during IC processing
As Si is an indirect band gap material, the PL generated by phonon assisted band-to-band (B2B) radiative recombination (of energy equal to energy gap of Si) is very weak; about 10 orders of magnitude lower than the exciting photon flux [1] . If crystallographic defects are present then at room temperature an additional broad defect PL peak is generated (DPL) with energy smaller than the band gap of Si [1] , [2] , [3] . At room temperature, defect-band PL intensity is orders of magnitude lower than the B2B intensity [1] .