Department of Physics, Clarendon Laboratory, University of Oxford , Parks Road, Oxford OX1 3PU, U.K.
Acc Chem Res. 2016 Jan 19;49(1):146-54. doi: 10.1021/acs.accounts.5b00411. Epub 2015 Dec 10.
Photovoltaic (PV) devices that harvest the energy provided by the sun have great potential as renewable energy sources, yet uptake has been hampered by the increased cost of solar electricity compared with fossil fuels. Hybrid metal halide perovskites have recently emerged as low-cost active materials in PV cells with power conversion efficiencies now exceeding 20%. Rapid progress has been achieved over only a few years through improvements in materials processing and device design. In addition, hybrid perovskites appear to be good light emitters under certain conditions, raising the prospect of applications in low-cost light-emitting diodes and lasers. Further optimization of such hybrid perovskite devices now needs to be supported by a better understanding of how light is converted into electrical currents and vice versa. This Account provides an overview of charge-carrier recombination and mobility mechanisms encountered in such materials. Optical-pump-terahertz-probe (OPTP) photoconductivity spectroscopy is an ideal tool here, because it allows the dynamics of mobile charge carriers inside the perovskite to be monitored following excitation with a short laser pulse whose photon energy falls into the range of the solar spectrum. We first review our insights gained from transient OPTP and photoluminescence spectroscopy on the mechanisms dominating charge-carrier recombination in these materials. We discuss that mono-molecular charge-recombination predominantly originates from trapping of charges, with trap depths being relatively shallow (tens of millielectronvolts) for hybrid lead iodide perovskites. Bimolecular recombination arises from direct band-to-band electron-hole recombination and is found to be in significant violation of the simple Langevin model. Auger recombination exhibits links with electronic band structure, in accordance with its requirement for energy and momentum conservation for all charges involved. We further discuss charge-carrier mobility values extracted from OPTP measurements and their dependence on perovskite composition and morphology. The significance of the reviewed charge-carrier recombination and mobility parameters is subsequently evaluated in terms of the charge-carrier diffusion lengths and radiative efficiencies that may be obtained for such hybrid perovskites. We particularly focus on calculating such quantities in the limit of ultra-low trap-related recombination, which has not yet been demonstrated but could be reached through further advances in material processing. We find that for thin films of hybrid lead iodide perovskites with typical charge-carrier mobilities of ∼30cm(2)/(V s), charge-carrier diffusion lengths at solar (AM1.5) irradiation are unlikely to exceed ∼10 μm even if all trap-related recombination is eliminated. We further examine the radiative efficiency for hybrid lead halide perovskite films and show that if high efficiencies are to be obtained for intermediate charge-carrier densities (n ≈ 10(14) cm(-3)) trap-related recombination lifetimes will have to be enhanced well into the microsecond range.
光 伏 (PV) 器件利用太阳能作为可再生能源具有很大的潜力,然而与化石燃料相比,太阳能发电的成本增加了,这阻碍了其普及。 混合卤化金属钙钛矿作为光伏电池中的低成本活性材料最近出现,其功率转换效率现已超过 20%。 通过改进材料处理和器件设计,仅在几年内就取得了快速进展。 此外,在某些条件下,混合钙钛矿似乎是良好的发光体,这为低成本发光二极管和激光器的应用带来了前景。 为了进一步优化这种混合钙钛矿器件,现在需要更好地了解光如何转化为电流,反之亦然。 本账户概述了在这些材料中遇到的载流子复合和迁移机制。 光泵太赫兹探针 (OPTP) 光电导光谱学是一种理想的工具,因为它可以在使用短激光脉冲激发后监测钙钛矿内部可移动载流子的动力学,该激光脉冲的光子能量落在太阳光谱的范围内。 我们首先回顾了从瞬态 OPTP 和光致发光光谱中获得的关于这些材料中载流子复合主导机制的见解。 我们讨论了单分子电荷复合主要源于电荷的俘获,对于混合碘化铅钙钛矿,陷阱深度相对较浅(几十毫电子伏特)。 双分子复合源于直接带隙电子-空穴复合,并且明显违反了简单的朗之万模型。 俄歇复合与电子能带结构有关,这符合其对所有参与电荷的能量和动量守恒的要求。 我们进一步讨论了从 OPTP 测量中提取的载流子迁移率值及其对钙钛矿组成和形态的依赖性。 随后,根据此类混合钙钛矿可能获得的载流子扩散长度和辐射效率,评估了所审查的载流子复合和迁移参数的重要性。 我们特别关注在与超低位陷相关的复合的极限下计算这些数量,尽管尚未证明这一点,但通过进一步改进材料处理可能达到这一点。 我们发现,对于典型载流子迁移率约为 30cm2/(V s)的混合碘化铅钙钛矿薄膜,即使消除了所有与位陷相关的复合,在太阳(AM1.5)辐照下,载流子扩散长度也不太可能超过约 10μm。 我们进一步研究了混合卤化铅钙钛矿薄膜的辐射效率,并表明如果要在中等载流子密度(n≈1014cm-3)下获得高效率,与位陷相关的复合寿命必须延长到微秒范围。