中间波段和串联混合太阳能电池材料的理论分析

Jongwon Lee, S. Dahal, C. Honsberg
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引用次数: 1

摘要

中间带(IB)太阳能电池的效率极限可以通过多个中间带器件的“串联”配置来提高。热力学模型表明,双叠串联IB器件的效率达到了六结串联太阳能电池的效率。与单叠或双叠串联相结合的IB效率具有类似的效率优势。此外,对可用于在串联配置中实现IB太阳能电池的材料的分析显示了与使用量子阱或量子点实现IB材料的能力相关的优点。对于单个IB太阳能电池,一个关键的困难是确定具有小价带偏移和大导带偏移(或相反)的势垒和量子阱材料。使用IB太阳能电池作为串联的底部太阳能电池允许更大范围的材料具有合适的势垒带隙和较小的理想导带偏移。这种结构的另一个理论优势是它避免了低带隙材料中pn结的极低开路电压;例如,6结串联太阳能电池的热力学最优带隙低于0.4 eV。我们提出了IB混合串联结构的热力学模型,该模型不假设不同太阳能电池之间的光谱选择性,并预测势垒/量子点结构在1000倍黑体辐射下的效率可高达60%至70%。
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Theoretical analysis for intermediate band and tandem hybrid solar cell materials
The efficiency limit of an intermediate band (IB) solar cell can be increased by a “tandem” configuration of multiple intermediate band devices. Thermodynamic models show that the efficiency of a two-stack tandem of IB devices achieves the efficiency of a six junction series connected solar cell. The efficiency of an IB in conjunction with a single or double stack tandem has similar efficiency advantages. Further, analysis of the materials which can be used to implement IB solar cells in a tandem configuration shows advantages relating to the ability to implement IB materials with quantum wells or quantum dots. For a single IB solar cell, a key difficulty is identifying materials for the barrier and the quantum well which have a small valence band offset and large conduction band offset (or the reverse). The use of an IB solar cell as the bottom solar cell of a tandem allows a larger range of materials with suitable barrier band gaps and a smaller ideal conduction band offset. A further theoretical advantage of such a structure is that it avoids the extremely low open circuit voltages achieved from pn junctions in low bandgap materials; for example, the thermodynamic optimum for a 6 junction tandem solar cell has its lowest bandgap below 0.4 eV. We present a thermodynamic model for IB hybrid tandem configurations which does not assume spectral selectivity among the different solar cells and predicts that a barrier/quantum dot structure can have an efficiency as high as 60 to 70 percent at 1000X blackbody radiation.
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