开路电压
钙钛矿(结构)
二极管
重组
光电子学
电压
光强度
扩散
化学
指数函数
分析化学(期刊)
物理
分子物理学
原子物理学
光学
结晶学
热力学
基因
数学分析
量子力学
生物化学
色谱法
数学
作者
Non Thongprong,Thidarat Supasai,Youyong Li,I‐Ming Tang,Nopporn Rujisamphan
标识
DOI:10.1002/ente.201901196
摘要
To analyze the dominant recombination, researchers often consider the diode ideality factor ( n id ), determined from the fitting of a semi‐log plot of light intensity–dependent open‐circuit voltage ( V oc (ln I/I 0 )) to a linear dependence. This value is called “ n id,Voc ”. Theoretically, n id is the exponential dependence factor in the recombination rate function of the split of quasi‐Fermi levels. This n id is called “ n id,C ”. Herein, correlations between n id,Voc , n id,C , and the dominant recombination are reconsidered using a validated numerical drift–diffusion model and a diode current analysis in perovskite solar cell devices having accumulations of charged defects near the carrier transporting interfaces. It is found that the interplay between the recombination processes affects the linearity of the V oc (ln I/I 0 ) plots. Devices having a single dominant recombination process exhibit V oc (ln I/I 0 ) plots that appear to be linear, resulting in n id,Voc ≈ n id,C of the dominant recombination. Conversely, bends in the V oc (ln I/I 0 ) curves indicate that different (multiple) recombination mechanisms dominate at different light intensities, so n id,Voc is an effective n id of the total diode current whose value is not consistent with any n id,C values. This work provides more understanding of n id and how to interpret a V oc ( lnI/I 0 ) curve more correctly for the insights into recombination mechanisms.
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