Grafel

Publications

New Donor-Acceptor polymers with a wide absorption range for photovoltaic applications. Elsevier Solar Energy 205, 211–220 (2020)

Publications Friday, 20 November 2020 00:00

M.L. Keshtova, S.A. Kuklina, I.O. Konstantinova, I.E. Ostapova,b, Zh. Xiec, Emmanuel N. Koukarasd, Rakesh Suthare, Ganesh D. Sharmae

a Institute of Organoelement Compounds of the Russian Academy of Sciences, Vavilova St., 28, 119991 Moscow, Russia
b Department of Physics of Polymers and Crystals, Faculty of Physics, M.V. Lomonosov Moscow State University, Leninskie Gory 1, 119991 Moscow, Russia
c Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, China
d Laboratory of Quantum and Computational Chemistry, Department of Chemistry, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece
e Department of Physics, The LNM Institute for Information Technology, Jamdoli, Jaipur 302017, India.

DOI: 10.1016/j.solener.2020.05.059

ABSTRACT

For conjugated polymers of interest in photovoltaic applications, control of the bandgap as well as the energy levels of the molecules are of great importance to improve the efficiency and performance of the resulting polymer solar cells. A general tactic for adjusting these properties via modification of the conjugated polymer structure is by using different and chosen molecular groups for copolymerization. This communication presents the synthesis of conjugated donor–acceptor type polymers that have the same benzotrithiophene (BTT) donor and different acceptor units, i.e. DPP and fluoro-carbazole substituted thieno[3,4-b]pyrazine (FCTP) denoted as P(BTT-DPP) (P1) and P(BTT-FCTP) (P2), respectively, and their photovoltaic performance using as donor, and non-fullerene acceptor (PDIF) in the bulk heterojunction active layer. The bandgaps as well as the HOMO and LUMO energy levels are effectively tuned. The P(BTT-FCTPZ) structure exhibits a smaller bandgap as compared to P(BTT-DPP) that results from the lower LUMO energy and higher HOMO energy due to the FCTP unit. Having optimized the active layers, the PSCs that were based on P(BTT-DPP) and P(BTT-FCTPZ) gave an overall power conversion efficiency of about 9.77% and 10.97%, respectively, using a wide bandgap PDIF non-fullerene acceptor, and 8.38% and 9.05, respectively, using PC71BM as electron acceptor.

 

Last modified on Monday, 07 March 2022 16:06