J. Hofstetter, R. Fraser, R. Jonczyk, A. Erşen, John Linton, A. Lorenz
{"title":"高电阻率p型无角多晶片的有效寿命超过1ms","authors":"J. Hofstetter, R. Fraser, R. Jonczyk, A. Erşen, John Linton, A. Lorenz","doi":"10.1109/PVSC40753.2019.9198964","DOIUrl":null,"url":null,"abstract":"Kerfless p-type wafers of varying resistivity are grown with Direct Wafer technology with precise control of dosing the Boron concentration in the melt. At very low Boron concentration, bulk resistivity values ≫100 Ω-cm are achieved and an effective lifetime above 1 ms is measured, corresponding to an estimated bulk lifetime around 2 ms. In contrast to ingot-based wafers, continuous growth using Direct Wafer technology produces a very tight resistivity distribution at any desired target resistivity, without variations caused by zone refining. In addition, the technology enables growth of 3D wafers, e.g. thin wafers with a thick frame that allows to maintain mechanical wafer strength. Thus, Direct Wafer product can be customized for a given solar cell architecture by growing each individual wafer at the optimum bulk resistivity and optimum thickness.","PeriodicalId":6749,"journal":{"name":"2019 IEEE 46th Photovoltaic Specialists Conference (PVSC)","volume":"14 1","pages":"1-4"},"PeriodicalIF":0.0000,"publicationDate":"2019-06-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Exceeding 1 ms effective lifetime in High High-Resistivity P-Type Kerfless Multi-crystalline Wafers\",\"authors\":\"J. Hofstetter, R. Fraser, R. Jonczyk, A. Erşen, John Linton, A. Lorenz\",\"doi\":\"10.1109/PVSC40753.2019.9198964\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Kerfless p-type wafers of varying resistivity are grown with Direct Wafer technology with precise control of dosing the Boron concentration in the melt. At very low Boron concentration, bulk resistivity values ≫100 Ω-cm are achieved and an effective lifetime above 1 ms is measured, corresponding to an estimated bulk lifetime around 2 ms. In contrast to ingot-based wafers, continuous growth using Direct Wafer technology produces a very tight resistivity distribution at any desired target resistivity, without variations caused by zone refining. In addition, the technology enables growth of 3D wafers, e.g. thin wafers with a thick frame that allows to maintain mechanical wafer strength. Thus, Direct Wafer product can be customized for a given solar cell architecture by growing each individual wafer at the optimum bulk resistivity and optimum thickness.\",\"PeriodicalId\":6749,\"journal\":{\"name\":\"2019 IEEE 46th Photovoltaic Specialists Conference (PVSC)\",\"volume\":\"14 1\",\"pages\":\"1-4\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-06-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2019 IEEE 46th Photovoltaic Specialists Conference (PVSC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PVSC40753.2019.9198964\",\"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 IEEE 46th Photovoltaic Specialists Conference (PVSC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PVSC40753.2019.9198964","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Exceeding 1 ms effective lifetime in High High-Resistivity P-Type Kerfless Multi-crystalline Wafers
Kerfless p-type wafers of varying resistivity are grown with Direct Wafer technology with precise control of dosing the Boron concentration in the melt. At very low Boron concentration, bulk resistivity values ≫100 Ω-cm are achieved and an effective lifetime above 1 ms is measured, corresponding to an estimated bulk lifetime around 2 ms. In contrast to ingot-based wafers, continuous growth using Direct Wafer technology produces a very tight resistivity distribution at any desired target resistivity, without variations caused by zone refining. In addition, the technology enables growth of 3D wafers, e.g. thin wafers with a thick frame that allows to maintain mechanical wafer strength. Thus, Direct Wafer product can be customized for a given solar cell architecture by growing each individual wafer at the optimum bulk resistivity and optimum thickness.