Integrating Ultrathin Bulk-Heterojunction Organic Semiconductor Intermediary for High-Performance Low-Bandgap Perovskite Solar Cells with Low Energy Loss

Integrating Ultrathin Bulk-Heterojunction Organic Semiconductor Intermediary for High-Performance Low-Bandgap Perovskite Solar Cells with Low Energy Loss
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DOI:
10.1002/adfm.201804427
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发表时间:
2018-10-17
影响因子:
19
通讯作者:
Li, Yongfang
Li, Yongfang
中科院分区:
材料科学1区
文献类型:
--
作者:
Xu, Guiying;Bi, Pengqing;Li, Yongfang

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混合锡铅钙钛矿被认为是最有前途的低带隙光伏材料,既追求单结太阳能电池的理论极限效率,又通过构建串联太阳能电池来打破Shockley-Queisser限制。然而,由于其严重的能量损失(E-loss),它们的功率转换效率(PCE)仍然落后于中带隙钙钛矿太阳能电池(pero-SC)。在此,将半导体本体异质结(BHJ)有机半导体(PBDB-T:ITIC)层用作空穴传输层和Sn-Pb基低带隙钙钛矿膜之间的中间体以使E损失最小化。结果发现,这种BHJ PBDB-T:ITIC中间体同时提供了一个级联的能量对齐的设备,促进高品质的锡铅钙钛矿薄膜的生长,并钝化钙钛矿表面的反位缺陷。以这种简单的方式,基于(FASnI(3))(0.6)(MAPbI(3))(0.4)(带隙接近1.25 eV)的pero-SC的E损耗显著降低到0.4 eV以下,导致0.86 V的高开路电压(V-oc)。结果,最佳的pero-SC显示出18.03%的显著改善的PCE,具有可忽略的J-V滞后和高稳定性。据了解,18.03%的PCE和0.86 V的V-oc是迄今为止低带隙pero-SC中的最高值。
Mixed tin (Sn)-lead (Pb) perovskite is considered the most promising low-bandgap photovoltaic material for both pursuing the theoretical limiting efficiency of single-junction solar cells and breaking the Shockley-Queisser limitation by constructing tandem solar cells. However, their power conversion efficiencies (PCEs) are still lagging behind those of medium-bandgap perovskite solar cells (pero-SCs) due to their serious energy loss (E-loss). Here, an ultrathin bulk-heterojunction (BHJ) organic semiconductor (PBDB-T:ITIC) layer is used as an intermediary between the hole transporting layer and Sn-Pb-based low-bandgap perovskite film to minimize E-loss. It is found that this BHJ PBDB-T:ITIC intermediary simultaneously provided a cascading energy alignment in the device, facilitated high-quality Sn-Pb perovskite film growth, and passivated the antisite defects of the perovskite surface. In this simple way, the E-loss of pero-SCs based on (FASnI(3))(0.6)(MAPbI(3))(0.4) (bandgap approximate to 1.25 eV) is dramatically reduced below 0.4 eV, leading to a high open-circuit voltage (V-oc) of 0.86 V. As a result, the best pero-SC showed a significantly improved PCE of 18.03% with negligible J-V hysteresis and high stability. As far as it is known, the PCE of 18.03% and V-oc of 0.86 V are the highest values among the low-bandgap pero-SCs to date.