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A dye – sensitized solar cell module with enhanced charge collection efficiency

机译:染料敏化太阳能电池模块,具有更高的电荷收集效率

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摘要

Intense research in the field of dye-sensitized solar cells (DSCs) brought them to a level of delivering ~13% efficiency (η) using mesoporous TiO2 particles, inorganic dyes, and redox electrolyte. High η and IPCEs are so far reported in devices of rather smaller area (≤ 0.2 cm2), a size that put limitations on the scalability of the device. On the other hand, large area modules (DSMs) are developed by up scaling the DSCs to give either added voltages (series connection), such as S –type, W–type and Z–type, or currents (parallel connection) with appreciable output voltage (~8 V) and current (~2 – 3 A), respectively, in separate devices of active areas in the 20 – 1000 cm2 range. The highest achieved in DSMs is ~ 8.2%, ~36% smaller than their laboratory scale devices. We note that such designs are invariably built in the form of interconnected TiO2 strips (≥ 3 cm2) and the photocurrent density (JSC) in these designs is merely 30 – 50 % then that of single cells. We have investigated the effects of DSC photoelectrode area upon its  and identified that, within the limits of our study, threshold area is the key in achieving the JSC and clearly not the expanded photoelectrode area as adopted conventionally in a DSM fabrication. Upon increasing the photoelectrode area, the  decreased biexponentially, the main contributor to which was the JSC. The upshots of the electrochemical studies revealed that the electrons from an area above a threshold are never collected due to a competition between electron lifetime (τn) and transit time (τd). We suggest that if larger electrodes are fabricated, then electrons from smaller spatial domains contribute to the short circuit current density. The diffusion length (Ln) in DSCs, which is defined as the distance travelled by electrons before recombining with the hole species in electrolyte, L= (Dnn)1/2, where Dn is the electron diffusivity, considered only film thickness so far. Our findings reveal that area of the electrode is also to be considered when the L is defined. Based on the insights, we fabricated alternative designs to build DSMs with increased charge collection (c). In our specially designed experiments, we altered the photoelectrode design by splitting the electrode into multiple fractions to restrict the electron diffusion pathways. We observed a correlation between the device physical dimensions and its charge collection efficiency via current-voltage and impedance spectroscopy measurements. Our electrode designs showed >50 % increased JSC due to shorter τd, higher recombination resistance and 20 – 50% higher c compared to the conventional ones despite their similar active volume (~3.36 × 10-4 cm3). If high efficiency DSCs is targeted using commercial TiO2 paste on account of its high specific surface area, results from our studies would be helpful in designing new device structures to build high efficiency DSMs
机译:染料敏化太阳能电池(DSC)领域的大量研究使它们使用介孔TiO2颗粒,无机染料和氧化还原电解质达到了约13%的效率(η)。迄今为止,在面积较小(≤0.2 cm2)的设备中报告了较高的η和IPCE,该尺寸限制了设备的可扩展性。另一方面,通过扩展DSC来开发大面积模块(DSM),以提供增加的电压(串联),例如S型,W型和Z型,或者具有可观电流的电流(并联)。分别在20 – 1000 cm2范围内的有效区域中的不同设备中分别输出电压(〜8 V)和电流(〜2 – 3 A)。在DSM中,最高的约为8.2%,比其实验室规模的设备小约36%。我们注意到,这样的设计总是以互连的TiO2条(≥3 cm2)的形式构建的,并且这些设计中的光电流密度(JSC)仅为单电池的30%至50%。我们研究了DSC光电极面积对其effects的影响,并确定在我们的研究范围内,阈值区域是实现JSC的关键,显然不是DSM制造中常规采用的扩展光电极面积。随着光电极面积的增加,bi呈双指数下降,其主要贡献者是JSC。电化学研究的结果表明,由于电子寿命(τn)和渡越时间(τd)之间的竞争,从未收集到超过阈值区域的电子。我们建议,如果制造更大的电极,则来自较小空间域的电子会导致短路电流密度。 DSC中的扩散长度(Ln)定义为电子在与电解质中的空穴种类重新结合之前所经过的距离,L =(Dnn)1/2,其中Dn是电子扩散率,仅考虑薄膜厚度,因此远。我们的发现表明,当定义了L时,也要考虑电极的面积。基于这些见解,我们制造了替代设计来构建具有更高电荷收集(c)的DSM。在我们特别设计的实验中,我们通过将电极分成多个部分以限制电子扩散路径,从而改变了光电极的设计。我们通过电流-电压和阻抗谱测量观察到器件物理尺寸与其电荷收集效率之间的相关性。我们的电极设计显示,尽管它们的活性体积相似(〜3.36×10-4 cm3),但与传统电极相比,τd较短,复合电阻更高,c高出20%至50%,这是因为它们的τd短,JSC增大了50%以上。如果由于高比表面积而使用市售TiO2浆料作为高效DSC的目标,我们的研究结果将有助于设计新的器件结构来构建高效DSM

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    Azhar Fakharuddin;

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  • 年度 2015
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