Star-Shaped Hole Transporting Materials with Triphenylamine Core for Perovskite Solar Cells with 12.38% Conversion Efficiency
An-Na Cho a, Hui-Seon Kim a, Nam-Gyu Park a, Xavier Sallenave b, Fabrice Goubard b, Thanh-Tuan Bui b
a Sungkyunkwan University, South Korea, 300 Cheoncheon-dong, Jangan-gu, Suwon, 440, Korea, Republic of
b Laboratoire de Physicochimie des Polymeres et des Interfaces, Universite de Cergy-Pontoise, 5 mail Gay Lussac, 95000 Neuville-sur-Oise
International Conference on Hybrid and Organic Photovoltaics
Proceedings of International Conference on Hybrid and Organic Photovoltaics 2015 (HOPV15)
Roma, Italy, 2015 May 11th - 13th
Organizer: Filippo De Angelis
Poster, An-Na Cho, 159
Publication date: 5th February 2015
Recently, variety of triphenylamine (TPA) units have been widely studied and showed efficient charge transport and good morphological stability. Here we report a new star-shaped hole transport material (HTM) BT41 (tris(4-(5-(4,4'-dimethoxydiphenylaminyl)-2-thiophenyl)phenyl)amine) (Figure 1) with TPA core and short pi-conjugated branch. BT41 was applied to CH3NH3PbI3 perovskite solar cell. Compared to the convetional spiro-MeOTAD HTM, BT41 showed 50mV higher open-circuit voltage (Voc) despite 0.08 eV higher HOMO level, which was due to less recombination at BT41/perovskite interface as confirmed by impedance study. It was found that photovoltaic performance was significantly affected by additives. Voc was improved in the presence of 4-tert-butylpyridine (TBP) and fill factor (FF) was improved when TBP was coupled with bis(trifluoromethane)sulfonimide lithium salt (Li-TFSI), whereas photocurrent density (Jsc) was hardly influenced by Li-TFSI concentration. Device performance with BT41 was also affected by surface morphology of perovskite, where flat surface was better in photovoltaic performance than rough surface with large cuboid crystals. This indicates that interfacial eneginnering is crucial in case of molecular BT41 HTM. The best photovoltaic performance incorporating BT41 demonstrated Jsc of 18.46 mA/cm2, Voc of 1.03 V and FF of 0.65, leading to overall power conversion efficiency of 12.38%.
Figure 1. Structure of BT41
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