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Cited 22 time in webofscience Cited 19 time in scopus
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Impact of grain boundary defect on performance of perovskite solar cell

Authors
Iftiquar, S.M.[Iftiquar, S.M.]Yi, J.[Yi, J.]
Issue Date
1-Jun-2018
Publisher
ELSEVIER SCI LTD
Keywords
Carrier recombination loss; Diode ideality factor; Grain boundary defect; Methyl ammonium lead halide perovskite material; Perovskite solar cell; Reverse saturation current density
Citation
MATERIALS SCIENCE IN SEMICONDUCTOR PROCESSING, v.79, pp.46 - 52
Indexed
SCIE
SCOPUS
Journal Title
MATERIALS SCIENCE IN SEMICONDUCTOR PROCESSING
Volume
79
Start Page
46
End Page
52
URI
https://scholarworks.bwise.kr/skku/handle/2021.sw.skku/19676
DOI
10.1016/j.mssp.2018.01.022
ISSN
1369-8001
Abstract
Methyl ammonium lead halide (MAPbI(3)) perovskite is a crystalline material. It shows interesting properties that are suitable for absorber layer of solar cell. An optimized solar cell requires 200-400 nm thick absorber layer. However, the thin absorber layer inevitably contains grain of crystallites and hence grain boundary (GB) defects. The GB defects affect device performance. Therefore, we theoretically investigated the effects of GB defects on performance of solar cells. In this simulation studies, we kept total mid-gap defect density (N-d) as constant at 4x10(17) cm(-3) but varied the GB defect density (GB(dd)) from 3x10(12) cm(-3) to 3x10(22) cm(-3), because of which, the observed short circuit current density (J(sc)) of the cells remain nearly unchanged, but the open circuit voltage (V-oc) and power conversion efficiency (PCE) decreased steadily, while the fill factor (FF) shows a different trend of variation in a region (Region-X, say) where the GB(dd) and the N-d were nearly equal. A further investigation reveals that in the Region-X, a transition happens from defect mediated recombination to GB mediated recombination, where the reverse saturation current density (J(0)) and diode ideality factor (n) of the solar cells, reduce sharply from 3.46x10(-13) A cm(-2) to 2.65x10(-19) A cm(-2) and 1.9 to 1.1, respectively for a cell with 200 nm thick absorber layer. For 400 nm thick absorber layer, reduction of these parameters was 1.96x10(-13) A cm(-2) to 1.20x10(-17) A cm(-2) and 1.8 to 1.2 respectively.
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