{"title":"a-Si-Ge:H合金的磷硼掺杂及其对p-i-n太阳能电池的影响","authors":"R. Arya, J. Newton, B. Fieselmann","doi":"10.1109/PVSC.1988.105660","DOIUrl":null,"url":null,"abstract":"The performance of single-junction a-SiGe:H p-i-n solar cells has been optimized by addressing the alloy composition of the n-layer, the importance of the i(a-SiGe:H)/n interface, and the modification of hole transport in the intrinsic layer by low-level boron doping. The dark conductivity of an a-SiGe:H n-layer was about one order of magnitude lower than that of an a-Si:H n-layer, with a difference of 0.092 eV in the activation energy. Devices with an a-Si:H n-layer have superior performance with higher short-circuit current and FF (fill factor). An inverse graded layer at the i/n interface further improves the FF. Low-level boron doping of the i-layer shifts the Fermi level and changes the charge state of the recombination centers, resulting in an improvement in the long-wavelength response of devices. This optimization has led to an a-SiGe:H solar cell with a conversion efficiency of 10.1% for a short-circuit current density of 20.1 mA/cm/sup 2/.<<ETX>>","PeriodicalId":10562,"journal":{"name":"Conference Record of the Twentieth IEEE Photovoltaic Specialists Conference","volume":"1 1","pages":"85-90 vol.1"},"PeriodicalIF":0.0000,"publicationDate":"1988-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Phosphorous and boron doping of a-Si-Ge:H alloys and its effect on p-i-n solar cells\",\"authors\":\"R. Arya, J. Newton, B. Fieselmann\",\"doi\":\"10.1109/PVSC.1988.105660\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The performance of single-junction a-SiGe:H p-i-n solar cells has been optimized by addressing the alloy composition of the n-layer, the importance of the i(a-SiGe:H)/n interface, and the modification of hole transport in the intrinsic layer by low-level boron doping. The dark conductivity of an a-SiGe:H n-layer was about one order of magnitude lower than that of an a-Si:H n-layer, with a difference of 0.092 eV in the activation energy. Devices with an a-Si:H n-layer have superior performance with higher short-circuit current and FF (fill factor). An inverse graded layer at the i/n interface further improves the FF. Low-level boron doping of the i-layer shifts the Fermi level and changes the charge state of the recombination centers, resulting in an improvement in the long-wavelength response of devices. This optimization has led to an a-SiGe:H solar cell with a conversion efficiency of 10.1% for a short-circuit current density of 20.1 mA/cm/sup 2/.<<ETX>>\",\"PeriodicalId\":10562,\"journal\":{\"name\":\"Conference Record of the Twentieth IEEE Photovoltaic Specialists Conference\",\"volume\":\"1 1\",\"pages\":\"85-90 vol.1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1988-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Conference Record of the Twentieth IEEE Photovoltaic Specialists Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PVSC.1988.105660\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Conference Record of the Twentieth IEEE Photovoltaic Specialists Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PVSC.1988.105660","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Phosphorous and boron doping of a-Si-Ge:H alloys and its effect on p-i-n solar cells
The performance of single-junction a-SiGe:H p-i-n solar cells has been optimized by addressing the alloy composition of the n-layer, the importance of the i(a-SiGe:H)/n interface, and the modification of hole transport in the intrinsic layer by low-level boron doping. The dark conductivity of an a-SiGe:H n-layer was about one order of magnitude lower than that of an a-Si:H n-layer, with a difference of 0.092 eV in the activation energy. Devices with an a-Si:H n-layer have superior performance with higher short-circuit current and FF (fill factor). An inverse graded layer at the i/n interface further improves the FF. Low-level boron doping of the i-layer shifts the Fermi level and changes the charge state of the recombination centers, resulting in an improvement in the long-wavelength response of devices. This optimization has led to an a-SiGe:H solar cell with a conversion efficiency of 10.1% for a short-circuit current density of 20.1 mA/cm/sup 2/.<>