Volume 38, Issue 8 pp. 817-822
Concise Report

Modification of Hole Transport Layers for Fabricating High Performance Non-fullerene Polymer Solar Cells

B. Hari Babu

B. Hari Babu

School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan, Shandong, 250100 China

ǂThese authors contributed equally to this work.

Search for more papers by this author
Chengkun Lyu

Chengkun Lyu

School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan, Shandong, 250100 China

ǂThese authors contributed equally to this work.

Search for more papers by this author
Hongwei Zhang

Hongwei Zhang

State Key Laboratory of Supramolecular Structure and Materials, Institute of Theoretical Chemistry, Jilin University, Changchun, Jilin, 130012 China

Search for more papers by this author
Zhihao Chen

Zhihao Chen

School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan, Shandong, 250100 China

Search for more papers by this author
Fenghong Li

Fenghong Li

State Key Laboratory of Supramolecular Structure and Materials, Institute of Theoretical Chemistry, Jilin University, Changchun, Jilin, 130012 China

Search for more papers by this author
Lin Feng

Corresponding Author

Lin Feng

School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan, Shandong, 250100 China

E-mail: [email protected]Search for more papers by this author
Xiao-Tao Hao

Xiao-Tao Hao

School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan, Shandong, 250100 China

ARC Centre of Excellence in Exciton Science, School of Chemistry, University of Melbourne, Parkville, Victoria, 3010 Australia

Search for more papers by this author
First published: 29 March 2020
Citations: 13

Summary of main observation and conclusion

Interfacial engineering is expected to be a feasible strategy to improve the charge transport properties of the hole transport layer (HTL), which is of crucial importance to boost the device performance of organic solar cells (OSCs). In this study, two types of alcohol soluble materials, 2,3,5,6-tetrafluoro-7,7,8,8-tetracyanoquinodimethane (F4-TCNQ) and di-tetrabutylammoniumcis–bis(isothiocyanato)bis (2,2’-bipyridyl-4,4’-dicarboxylato) ruthenium(II) (N719) dye were selected as the dopant for HTL. The doping of F4-TCNQ and N719 dye in poly (ethylenedioxythiophene):poly(styrene sulfonate) (PEDOT:PSS) with and without integrating a graphene quantum-dots (G-QDs) layer has been explored in poly[[2,6′-4-8-di(5-ethylhexylthienyl)benzo[1,2-b:3,3-b]dithiophene][3-fluoro-2[(2-ethylhexyl)carbonyl]thieno[3,4-b]thio-phenediyl:(2,2′-((2Z,2′Z)-(((4,4,9, 9-tetrakis(4-hexylphenyl)-4,9-dihydro-s-indaceno[1,2-b:5,6-b′]dithiophene-2,7-diyl)bis(4-((2-ethylhexyl)oxy)thiophene-5,2-diyl))bis(methanylylidene))bis(5,6-difluoro-3-oxo-2,3-dihydro-1H-indene-2,1-diylidene))dimalononitrile (PTB7-Th:IEICO-4F) OSCs. The power conversion efficiency of the non-fullerene OSCs has been increased to 10.12% from 8.84%. The influence of HTL modification on the nano-morphological structures and photophysical properties is analyzed based on the comparative studies performed on the control and modified devices. The use of chemical doping and bilayer strategy optimizes the energy level alignment, nanomorphology, hole mobility, and work-function of HTL, leading to considerable reduction of the leakage current and recombination losses. Our work demonstrates that the doping of HTL and the incorporation of G-QDs layer to constitute a bilayer HTL is an promising strategy to fabricate high performance non-fullerene polymer solar cells

The full text of this article hosted at iucr.org is unavailable due to technical difficulties.