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  4. Simple mono-halogenated perylene diimides as non-fullerene electron transporting materials in inverted perovskite solar cells with ZnO nanoparticle cathode buffer layers
 
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Simple mono-halogenated perylene diimides as non-fullerene electron transporting materials in inverted perovskite solar cells with ZnO nanoparticle cathode buffer layers

Journal
Journal of Materials Chemistry A
Journal Volume
5
Journal Issue
25
Pages
12811-12821
Date Issued
2017
Author(s)
Wu, J.-L.
Huang, W.-K.
Chang, Y.-C.
Tsai, B.-C.
Hsiao, Y.-C.
Chang, C.-Y.
Chen, C.-T.  
DOI
10.1039/c7ta02617j
URI
https://www.scopus.com/inward/record.uri?eid=2-s2.0-85021650277&doi=10.1039%2fc7ta02617j&partnerID=40&md5=706809f657e7abb674029605e7778c9f
https://scholars.lib.ntu.edu.tw/handle/123456789/415862
Abstract
We have synthesized and characterized three perylene diimides, X-PDI, where X = H, F, or Br. These three compounds have been tested for the substitution of [6,6]-phenyl C61 butyric acid methyl ester (PC61BM) in inverted perovskite solar cells (PVSCs). Although the efficiency of PDI derivative-based conventional PVSCs is as high as 17.6% (J. Mater. Chem. A, 2016, 4, 8724), the corresponding performance of inverted PVSCs is still lagging behind and improvement is necessary. For electron accepting (from CH3NH3PbI3 perovskite) and electron transporting properties of the materials, UV-visible absorption spectroscopy, electrochemical cyclic voltammetry, direct current conductivity, space-charge limited current (SCLC) electron mobility, atomic force microscopy (AFM) surface morphology, and photoluminescence (PL) spectroscopy gauging charge-trapping have been studied. The HOMO/LUMO energy levels are 5.94/4.00, 5.83/3.96, 6.00/3.97, and 5.48/3.73 eV for H-PDI, F-PDI, Br-PDI, and PC61BM, respectively. Direct current conductivities of H-PDI, F-PDI, Br-PDI, and PC61BM are 8.71 × 10-8, 1.18 × 10-9, 2.2 × 10-6, and 8.42 × 10-6 S cm-1, respectively. The SCLC electron mobility of H-PDI, F-PDI, Br-PDI, and PC61BM are 1.12 × 10-4, 8.31 × 10-6, 1.08 × 10-3, and 5.00 × 10-3 S cm-1, respectively. PL spectroscopy of CH3NH3PbI3 perovskite provides emission at wavelength of 781 nm, which is the same as for the perovskite layer covered with a thin film of H-PDI or F-PDI. However, the emission wavelength was blue-shifted to 773-774 nm when the perovskite layer was covered with a thin film of Br-PDI or PC61BM. Using UV-visible absorption spectroscopy, the solubility (in chloroform) was determined as 1.2 × 10-2, 8.7 × 10-2 and >10-1 mol L-1 for F-PDI, H-PDI, and Br-PDI, respectively. In thin film state, UV-visible absorption spectroscopy indicated that the extent of molecular aggregation was F-PDI ≫ H-PDI > Br-PDI, which is consistent with the AFM-estimated root-mean-square roughness of F-PDI > H-PDI > Br-PDI ∼ PC61BM. Without the solution processed ZnO NP cathode buffer layer (CBL), the power conversion efficiency (PCE) of H-PDI, F-PDI, Br-PDI, and PC61BM PVSCs is ∼1%, ∼0%, 3.2%, and 4.1%, respectively. With the ZnO NP CBL, PCE is ∼7.8%, ∼0%, 10.5%, and 11.1% for H-PDI, F-PDI, Br-PDI, and PC61BM PVSCs, respectively. Through this study, we have demonstrated that the simple mono-bromine substituted perylene diimide (Br-PDI), is solution processable and has potential for use as a non-fullerene electron accepting and electron transporting material in inverted PVSCs.
SDGs

[SDGs]SDG7

Type
journal article

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