MXenes with tunable work functions and their application as electron- and hole-transport materials in non-fullerene organic solar cells

• Published in: Journal of materials chemistry. A, Materials for energy and sustainability Materials for energy and sustainability, 2019, Vol.7 (18), p.11160-11169
• Main Authors: Yu, Zhimeng, Feng, Wei, Lu, Wanheng, Li, Bichen, Yao, Hongyan, Zeng, Kaiyang, Ouyang, Jianyong
• Format: Article
• Language: English
• Subjects: Batteries; Buffers; Catalysis; Charge materials; Collection; Electrical conductivity; Electrical resistivity; Electrons; Energy conversion efficiency; Fullerenes; MXenes; Optoelectronic devices; Organic chemistry; Ozonation; Photovoltaic cells; Solar cells; Two dimensional materials; Work functions
• ISSN: 2050-7488; 2050-7496
• DOI: 10.1039/C9TA01195A

MXenes as 2D materials have attracted great attention due to their high electrical conductivity, high surface area, high transparency in the visible range and high hydrophilicity. They have been investigated in devices and systems including batteries, supercapacitors, and sensors as well as in catalysis but not in optoelectronic devices. In this work, we studied the application of Ti 3 C 2 T x for electron and hole collection in organic solar cells (OSCs). The work function of Ti 3 C 2 T x can be increased by a UV–ozone treatment and decreased through a treatment with N 2 H 4 . It can be thus tuned in a range from 4.08 to 4.95 eV. MXene films with different work functions are studied as electron and hole collection buffer materials for non-fullerene organic solar cells (OSCs) with poly[(2,6-(4,8-bis(5-(2-ethylhexyl)thiophen-2-yl)-benzo[1,2- b :4,5- b ′]dithiophene))- alt -(5,5-(1′,3′-di-2-thienyl-5′,7′-bis(2-ethylhexyl)benzo[1′,2′- c :4′,5′- c ′]dithiophene-4,8-dione))] (PBDB-T) and 3,9-bis(2-methylene-(3-(1,1-dicyanomethylene)-indanone))-5,5,11,11-tetrakis(4-hexylphenyl)-dithieno[2,3- d :2′,3′- d ′]-s-indaceno[1,2- b :5,6- b ′]dithiophene (ITIC) as the active materials. The OSCs with MXenes for electron or hole collection layers can exhibit a power conversion efficiency of 9.06% or 9.02%. These efficiencies are comparable to those obtained using conventional charge-collection buffer materials.