{"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}
引用次数: 4
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.