K. Kataoka, S. Tajima, M. Umehara, N. Takahashi, N. Isomura, Kosuke Kitazumi, Y. Kimoto
{"title":"利用硬x射线光电子能谱测量Cu 2 znsns4光伏电池的能带位置以实现高转换效率","authors":"K. Kataoka, S. Tajima, M. Umehara, N. Takahashi, N. Isomura, Kosuke Kitazumi, Y. Kimoto","doi":"10.1380/JSSSJ.38.565","DOIUrl":null,"url":null,"abstract":"For the Cu 2 ZnSnS 4 (CZTS) photovoltaic (PV) cells with a common structure of the window-layer (WL) / buffer-layer (BL) / absorbing-layer (AL), the band offset and band slope were measured by hard x-ray photoelectron spectroscopy. In view of the efficient transport of photo-excited free-electrons from CZTS-ALs to WLs via CdS-BLs, the conversion efficiency of the PV cells would be significantly affected by the band offset at BLs / ALs interface and the band slope in BLs. For the CZTS PV cells with a relatively high conversion efficiency of 9.4 % , the conduction band offset at CdS-BLs / CZTS-ALs interface was estimated to be 0.1 ± 0.1 eV with a cliff-type, and the band slope in CdS-BLs was estimated to be 0.5 ± 0.1 eV (downward slope to WLs) in the case of ZnO : Ga-WL. Absence of CB barrier at BLs / ALs interface and larger downward band slope in BLs to WLs are essential for higher conversion efficiency of the CZTS PV cells.","PeriodicalId":13075,"journal":{"name":"Hyomen Kagaku","volume":"17 1","pages":"565-570"},"PeriodicalIF":0.0000,"publicationDate":"2017-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Measurements of Energy Band Positions Using Hard X-ray Photoelectron Spectroscopy Aimed at Achieving High Conversion Efficiency Cu 2 ZnSnS 4 Photovoltaic Cells\",\"authors\":\"K. Kataoka, S. Tajima, M. Umehara, N. Takahashi, N. Isomura, Kosuke Kitazumi, Y. Kimoto\",\"doi\":\"10.1380/JSSSJ.38.565\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"For the Cu 2 ZnSnS 4 (CZTS) photovoltaic (PV) cells with a common structure of the window-layer (WL) / buffer-layer (BL) / absorbing-layer (AL), the band offset and band slope were measured by hard x-ray photoelectron spectroscopy. In view of the efficient transport of photo-excited free-electrons from CZTS-ALs to WLs via CdS-BLs, the conversion efficiency of the PV cells would be significantly affected by the band offset at BLs / ALs interface and the band slope in BLs. For the CZTS PV cells with a relatively high conversion efficiency of 9.4 % , the conduction band offset at CdS-BLs / CZTS-ALs interface was estimated to be 0.1 ± 0.1 eV with a cliff-type, and the band slope in CdS-BLs was estimated to be 0.5 ± 0.1 eV (downward slope to WLs) in the case of ZnO : Ga-WL. Absence of CB barrier at BLs / ALs interface and larger downward band slope in BLs to WLs are essential for higher conversion efficiency of the CZTS PV cells.\",\"PeriodicalId\":13075,\"journal\":{\"name\":\"Hyomen Kagaku\",\"volume\":\"17 1\",\"pages\":\"565-570\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2017-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Hyomen Kagaku\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1380/JSSSJ.38.565\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Hyomen Kagaku","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1380/JSSSJ.38.565","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Measurements of Energy Band Positions Using Hard X-ray Photoelectron Spectroscopy Aimed at Achieving High Conversion Efficiency Cu 2 ZnSnS 4 Photovoltaic Cells
For the Cu 2 ZnSnS 4 (CZTS) photovoltaic (PV) cells with a common structure of the window-layer (WL) / buffer-layer (BL) / absorbing-layer (AL), the band offset and band slope were measured by hard x-ray photoelectron spectroscopy. In view of the efficient transport of photo-excited free-electrons from CZTS-ALs to WLs via CdS-BLs, the conversion efficiency of the PV cells would be significantly affected by the band offset at BLs / ALs interface and the band slope in BLs. For the CZTS PV cells with a relatively high conversion efficiency of 9.4 % , the conduction band offset at CdS-BLs / CZTS-ALs interface was estimated to be 0.1 ± 0.1 eV with a cliff-type, and the band slope in CdS-BLs was estimated to be 0.5 ± 0.1 eV (downward slope to WLs) in the case of ZnO : Ga-WL. Absence of CB barrier at BLs / ALs interface and larger downward band slope in BLs to WLs are essential for higher conversion efficiency of the CZTS PV cells.