{"title":"PECVD生长n-i-p硅纳米线太阳能电池的制备","authors":"M. Adachi, K. Karim","doi":"10.1109/PVSC.2010.5616926","DOIUrl":null,"url":null,"abstract":"Silicon nanowires have been shown to have strong light trapping properties making them a promising photovoltaic material. In this study, silicon nanowires, grown by RF plasma enhanced chemical vapor deposition (PECVD), are incorporated as the absorbing layer in n-i-p solar cells. Silicon nanowires are fabricated at a temperature of 375 °C by Vapor Liquid Solid (VLS) method. Nanowire solar cells have an average specular reflectance of 6.3% as compared to 22.6% for the thin film amorphous silicon (a-Si) device (over λ = 350 nm − 750 nm). Similarly the average diffuse reflectance of the nanowire devices is 4.9% as compared to 9.4% for the thin film a-Si device. External quantum efficiency measurements indicate the largest contributor to collection efficiency losses is from the catalyst impurity used for nanowire growth.","PeriodicalId":6424,"journal":{"name":"2010 35th IEEE Photovoltaic Specialists Conference","volume":"47 1","pages":"003302-003305"},"PeriodicalIF":0.0000,"publicationDate":"2010-06-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":"{\"title\":\"Fabrication of PECVD grown n-i-p silicon nanowire solar cells\",\"authors\":\"M. Adachi, K. Karim\",\"doi\":\"10.1109/PVSC.2010.5616926\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Silicon nanowires have been shown to have strong light trapping properties making them a promising photovoltaic material. In this study, silicon nanowires, grown by RF plasma enhanced chemical vapor deposition (PECVD), are incorporated as the absorbing layer in n-i-p solar cells. Silicon nanowires are fabricated at a temperature of 375 °C by Vapor Liquid Solid (VLS) method. Nanowire solar cells have an average specular reflectance of 6.3% as compared to 22.6% for the thin film amorphous silicon (a-Si) device (over λ = 350 nm − 750 nm). Similarly the average diffuse reflectance of the nanowire devices is 4.9% as compared to 9.4% for the thin film a-Si device. External quantum efficiency measurements indicate the largest contributor to collection efficiency losses is from the catalyst impurity used for nanowire growth.\",\"PeriodicalId\":6424,\"journal\":{\"name\":\"2010 35th IEEE Photovoltaic Specialists Conference\",\"volume\":\"47 1\",\"pages\":\"003302-003305\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2010-06-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"5\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2010 35th IEEE Photovoltaic Specialists Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PVSC.2010.5616926\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2010 35th IEEE Photovoltaic Specialists Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PVSC.2010.5616926","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Fabrication of PECVD grown n-i-p silicon nanowire solar cells
Silicon nanowires have been shown to have strong light trapping properties making them a promising photovoltaic material. In this study, silicon nanowires, grown by RF plasma enhanced chemical vapor deposition (PECVD), are incorporated as the absorbing layer in n-i-p solar cells. Silicon nanowires are fabricated at a temperature of 375 °C by Vapor Liquid Solid (VLS) method. Nanowire solar cells have an average specular reflectance of 6.3% as compared to 22.6% for the thin film amorphous silicon (a-Si) device (over λ = 350 nm − 750 nm). Similarly the average diffuse reflectance of the nanowire devices is 4.9% as compared to 9.4% for the thin film a-Si device. External quantum efficiency measurements indicate the largest contributor to collection efficiency losses is from the catalyst impurity used for nanowire growth.