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Photovoltaic cells made from conjugated polymers infiltrated into ordered nanoporous hosts.

机译:由共轭聚合物制成的光伏电池渗透到有序的纳米多孔宿主中。

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Semiconducting (conjugated) polymers have several properties which make them ideal candidates for use in low-cost photovoltaic (PV) cells, including their typically high (105 cm-1) optical absorption coefficients, their ability to be cast from solution using a variety of wet-processing techniques, and the ability to tune their band gap. While most approaches for making conjugated polymer-based PV cells involve randomly intermixing the polymers with electron acceptors that act as sites for exciton dissociation, we have sought to obtain a more optimized morphology of the blended materials through a self-assembly technique. In the first half of this dissertation, we describe our preliminary attempts to make PV cells from conjugated polymers infiltrated into a self-assembled mesoporous titanic (TiO 2) electron acceptor that is ordered on the nanometer length scale. We first present a procedure for fabricating films of mesoporous TiO 2 and then show how its pores can be filled with a conjugated polymer, regioregular poly(3-hexylthiophene) (P3HT). In these films we have achieved precise control of the morphology of the two materials that has not yet been achieved elsewhere. However, as discussed subsequently, the photovoltaic performance of these films has not yet reached the level achieved by other types of conjugated polymer-based PV cells, with a maximum achieved power efficiency of approximately 0.45%.; In the second half of this dissertation, we embark on a more fundamental study of the materials requirements for efficient polymer photovoltaics, including models that show how the maximum achievable power efficiency is limited by energy loss during forward electron transfer, and how the maximum achievable photocurrent is limited by the limiting carrier mobility and back electron transfer. Our modeling suggests that, for a back recombination time constant of 1 mus, a limiting carrier mobility of 10-3--10 -2 cm2/Vs is required in order to achieve a large photocurrent across a fairly broad range of absorbed wavelengths. We then show how these mobility values can be achieved in a conjugated polymer through the vertical alignment of the chains of the polymer with respect to the plane of the substrate. These measurements were performed by infiltrating P3HT into a vertical-channel anodic alumina template.
机译:半导体(共轭)聚合物具有多种特性,使其成为低成本光伏(PV)电池的理想候选材料,包括其典型的高(105 cm-1)光吸收系数,使用多种溶液从溶液中浇铸的能力。湿法加工技术以及调节其带隙的能力。虽然大多数用于制造基于共轭聚合物的PV电池的方法都涉及将聚合物与电子受体随机混合,这些电子受体充当激子离解的位点,但我们已寻求通过自组装技术获得更优化的混合材料形态。在本论文的前半部分,我们描述了我们的初步尝试,该方法是将共轭聚合物渗透到自组装的介孔钛(TiO 2)电子受体中制成光伏电池,该纳米级有序排列。我们首先介绍一种制造介孔TiO 2薄膜的方法,然后说明如何用共轭聚合物(规则区域性聚(3-己基噻吩)(P3HT))填充其孔。在这些薄膜中,我们已经实现了对两种材料形态的精确控制,这是其他地方尚未实现的。然而,如随后所讨论的,这些膜的光伏性能尚未达到其他类型的基于共轭聚合物的PV电池所达到的水平,最大实现的功率效率约为0.45%。在本文的后半部分,我们将对高效聚合物光伏材料的材料要求进行更基础的研究,其中包括一些模型,这些模型显示出最大可实现的功率效率如何受到正向电子转移过程中的能量损耗的限制,以及最大可实现的光电流如何受限制的载流子迁移率和反向电子转移的限制。我们的模型表明,对于1 mus的反向重组时间常数,为了在相当宽的吸收波长范围内获得大的光电流,需要限制的载流子迁移率为10-3--10 -2 cm2 / Vs。然后,我们展示了如何通过聚合物链相对于基材平面的垂直排列在共轭聚合物中实现这些迁移率值。通过将P3HT渗透到垂直通道阳极氧化铝模板中来执行这些测量。

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