缓慢的空穴扩散限制了基于 P1 染料的 p 型染料敏化太阳能电池的效率

IF 3.2 Q2 CHEMISTRY, PHYSICAL
Energy advances Pub Date : 2024-07-02 DOI:10.1039/D4YA00271G
Maria B. Brands, Olivier C. M. Lugier, Kaijian Zhu, Annemarie Huijser, Stefania Tanase and Joost N. H. Reek
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引用次数: 0

摘要

氧化镍电极被广泛应用于对型染料敏化太阳能电池(DSSC)和光电化学电池中,但由于过多的电荷重组,这些器件的效率仍然太低,无法进行商业应用。为了了解哪些因素会导致电荷重组,我们在基准 P1 p-DSSC 中研究了具有不同数量氧化镍层的电极。我们用四层氧化镍(0.134%)获得了最高效的 DSSC,并通过染料负载研究和操作中光电化学瞬态光谱进一步了解了这一最佳值。这些结果表明,NiO 层数越多,光收集效率(ηLH)越高,但空穴收集效率(ηCC)却越低,当 NiO 层数达到 4 层时,光收集效率达到最高。ηCC随着氧化镍层数的增加而降低,这是由于空穴收集时间延长,最终限制了整体效率。值得注意的是,重组率与氧化镍层数无关,与在更高效的 n 型 DSSC 类似物中观察到的重组率相似,但空穴收集速度要慢一个数量级。因此,随着镍氧化物层数的增加,ηLH的有益增加不再能抵消由于空穴收集速度慢而导致的ηCC的减少,从而导致太阳能电池的整体效率在镍氧化物层数达到四层时达到最高。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Slow hole diffusion limits the efficiency of p-type dye-sensitized solar cells based on the P1 dye†

Slow hole diffusion limits the efficiency of p-type dye-sensitized solar cells based on the P1 dye†

NiO electrodes are widely applied in p-type dye-sensitized solar cells (DSSCs) and photoelectrochemical cells, but due to excessive charge recombination, the efficiencies of these devices are still too low for commercial applications. To understand which factors induce charge recombination, we studied electrodes with a varying number of NiO layers in benchmark P1 p-DSSCs. We obtained the most efficient DSSCs with four layers of NiO (0.134%), and further insights into this optimum were obtained via dye loading studies and in operando photoelectrochemical immittance spectroscopy. These results revealed that more NiO layers led to an increasing light harvesting efficiency (ηLH), but a decreasing hole collection efficiency (ηCC), giving rise to the maximum efficiency at four NiO layers. The decreasing ηCC with more NiO layers is caused by longer hole collection times, which ultimately limits the overall efficiency. Notably, the recombination rates were independent of the number of NiO layers, and similar to those observed in the more efficient n-type DSSC analogues, but hole collection was an order of magnitude slower. Therefore, with more NiO layers, the beneficial increase in ηLH can no longer counteract the decrease in ηCC due to slow hole collection, resulting in the overall efficiency of the solar cells to maximize at four NiO layers.

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