{"title":"边缘照明梯度间隙太阳能电池的分析","authors":"J. Parrott","doi":"10.1049/IJ-SSED:19780029","DOIUrl":null,"url":null,"abstract":"It has been established that even under ideal conditions the efficiency of a semiconductor photovoltaic cell with a single energy gap cannot exceed approximately 30%. One possible configuration for avoiding this limitation is the edge-illuminated graded-gap solar cell, in which the plane of the p-n junction is parallel to the incident radiation and the gap is graded from a larger value at the illuminated surface to a smaller at the back. Calculations were carried out for (a) fixed front-surface energy gap and variable backsurface gap, and (b) fixed back-surface gap and variable front-surface gap. In each case the fixed gap was 1.47 eV. The best result was an increase of theoretical efficiency from 27.2 to 28.3% for the first case with a back surface gap of l.27eV at a thousand suns. To increase the efficiency further it would be necessary to segment the device.","PeriodicalId":127114,"journal":{"name":"Iee Journal on Solidstate and Electron Devices","volume":"98 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1978-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"Analysis of an edge-illuminated graded-gap solar cell\",\"authors\":\"J. Parrott\",\"doi\":\"10.1049/IJ-SSED:19780029\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"It has been established that even under ideal conditions the efficiency of a semiconductor photovoltaic cell with a single energy gap cannot exceed approximately 30%. One possible configuration for avoiding this limitation is the edge-illuminated graded-gap solar cell, in which the plane of the p-n junction is parallel to the incident radiation and the gap is graded from a larger value at the illuminated surface to a smaller at the back. Calculations were carried out for (a) fixed front-surface energy gap and variable backsurface gap, and (b) fixed back-surface gap and variable front-surface gap. In each case the fixed gap was 1.47 eV. The best result was an increase of theoretical efficiency from 27.2 to 28.3% for the first case with a back surface gap of l.27eV at a thousand suns. To increase the efficiency further it would be necessary to segment the device.\",\"PeriodicalId\":127114,\"journal\":{\"name\":\"Iee Journal on Solidstate and Electron Devices\",\"volume\":\"98 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1978-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Iee Journal on Solidstate and Electron Devices\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1049/IJ-SSED:19780029\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Iee Journal on Solidstate and Electron Devices","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1049/IJ-SSED:19780029","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Analysis of an edge-illuminated graded-gap solar cell
It has been established that even under ideal conditions the efficiency of a semiconductor photovoltaic cell with a single energy gap cannot exceed approximately 30%. One possible configuration for avoiding this limitation is the edge-illuminated graded-gap solar cell, in which the plane of the p-n junction is parallel to the incident radiation and the gap is graded from a larger value at the illuminated surface to a smaller at the back. Calculations were carried out for (a) fixed front-surface energy gap and variable backsurface gap, and (b) fixed back-surface gap and variable front-surface gap. In each case the fixed gap was 1.47 eV. The best result was an increase of theoretical efficiency from 27.2 to 28.3% for the first case with a back surface gap of l.27eV at a thousand suns. To increase the efficiency further it would be necessary to segment the device.