Organic solar cells based on non-fullerene acceptors of nine fused-ring by modifying end groups
Graphical abstract
Introduction
In the past few years, organic solar cells have developed rapidly, and bulk hetero-junction (BHJ) [1] organic solar cells (OSCs) are one of the most commonly used device structures based on p-type organic semiconductor electron donors blended with n-type organic semiconductor electron acceptors as active layer and have been achieved great progress [[2], [3], [4], [5], [6], [7]]. It is attribute to the development of high performance donors [[8], [9], [10], [11], [12]], acceptors [[13], [14], [15], [16], [17], [18]] and electrode buffer layer materials [19,20]. For acceptor materials, they are classified into fullerene acceptors such as PCBM [[21], [22], [23], [24]] and non-fullerene acceptors. Non-fullerene acceptors (NFAs) are mainly small molecule acceptor (SMAs) [[25], [26], [27]] and polymer acceptors. Compared with polymer acceptors, the SMAs have the advantages of strong absorption, adjustable energy level, high carrier mobility, excellent phase separation morphology, and easy modification. Therefore, the development of polymer acceptor materials relative to SMAs are jog along. At the same time, n-type donors also play an important role in organic solar cells as hole transport carriers for photovoltaic devices, while P3HT is the most representative donor photovoltaic material [28,29]. To produce a high performance OPVs, the most important are the match of the HOMO level of donors and the LUMO level of acceptors, high and balanced charge-carrier mobility, and complementary absorption bands in the Vis-NIR range of donors and acceptors. In addition, both the material composition ratio of the blend films and the morphology of the active layer affect the power conversion efficiencies (PCEs) of the OPVs.
In the last ten years, the A-D-A type fused-ring SMAs have received widespread attention from researchers due to its advantages such as adjustable energy levels and strong absorption, its rapid development has greatly promoted the development of OSCs and achieved high efficiency. For example, zhan’ group reported a series of A-D-A type SMAs [[30], [31], [32], [33]], such as IDIC, ITIC etc. For most reported SMAs, the absorption wavelength of the electron acceptors were lower than 800 nm, while the PCEs of the OSCs after matching the appropriate polymer donor materials could exceed 13%. Recently, the non-fullerene small molecule acceptor Y6 that synthesized by Zou and coworkers has an absorption peak exceeding 800 nm [34]. At the same time, Y6 has a HOMO level of −5.65 eV and a LUMO level of −4.10 eV, after matching with a polymer donor PM6, a high PCE of 15.7% was obtained, which is one of the most efficient acceptor materials so far.
In this paper, we plan to synthesize SMAs with near-infrared absorption based on benzodithiophene (BDT) and benzothiadiazole (BT) to improve the efficiency of OSCs. BDT has good symmetry, the molecular conformation presents a planar conjugated structure and small steric hindrance, which is a proven excellent donor unit and it could improve the electron mobility of SMAs [[35], [36], [37], [38], [39], [40], [41]]. Based on the above considerations, we designed and synthesized four SMAs based on a new benzodithiophene-pyrrolobenzothiadiazole central nine fused-ring unit. Firstly, 4,8-bis(2-ethylhexyloxy)benzo [1,2-b:4,5-b'] dithiophene (BDT-OEH) contains four alkoxy side chains, which can effectively improve the solubility of SMAs. Then, three different end groups of 2-(5,6-difluoro-3-oxo-2,3-dihydro-1H-inden-1-ylidene) malononitrile (2FIC), 3-(dicyanomethylene)indian-1-one (IC) and 2-(3-ethyl-4-oxo-thiazolidin-2-ylidene) malononitrile (RCN) were used to adjust the light absorption and energy levels of SMAs. In addition, we also added a π-bridge between the central core and the end group to adjust the performance. Finally, we obtained four SMAs, X94FIC, X9IC, X9Rd and X9T4FIC (Scheme 1). For X94FIC, X9IC and X9T4FIC, they were found to have narrow band gaps of 1.41 eV, 1.47 eV, and 1.47 eV, respectively, and X9Rd showed a wide band gap of 1.71 eV. In particular, the light absorption band of X94FIC reached an amazing 1000 nm, while X9IC and X9T4FIC also have a photo-response to 900 nm, which is beneficial for improving the PCE of OCSs.
Section snippets
Materials and methods
Toluene, tetrahydrofuran, dichloromethane and DMF were used after water removal strictly. All experimental drugs were reagent-grade chemicals purchased from formal commercial sources, and used directly unless specified. The compounds from each synthesis steps were purified by extraction, silica gel column chromatography and recrystallization. The chemical structures of the experimental products were determined by nuclear magnetic resonance spectra (NMR), which were measured on an Avance DPX-400
Synthesis and thermogravimetric
All synthetic routes are shown in Scheme 1. In order to obtain the target acceptor molecules, a series of routine reactions were applied, such as Stille coupling, Suzuki reaction, and Knoevenagel condensation reaction. First, one side of the BDT was protected with trimethylsilane and then a trimethylstannane on the other side. The compound 3 was coupled with 4,7-dibromo-5,6-dinitrobenzo [c] [1,2,5]thiadiazole, and then subjected to an N-hybrid ring reaction. The obtained unpurified compound 5
Conclusions
In summary, we designed and synthesized four small molecule acceptors X94FIC, X9IC, X9Rd, and X9T4FIC with different end groups under the same fused-ring core. A series of characterization and testing methods were used to analyze the thermogravimetric analysis, light absorption, photoelectric properties and film morphology of SMAs. Compared with the other three SMAs, X94FIC achieved the highest PCE of 7.08% after matching the donor PBDB-T. X94FIC obtained the highest Jsc due to its red-shifted
Declaration of competing interest
There are no conflicts to declare.
Acknowledgement
This work was supported by the National Science Foundation of China (Grants Nos. 21875204, 21805236, 21574144, 51773212, 61705240 and 21674123), the National Science Fund for Distinguished Young Scholars (21925506), the National Key R&D Program of China (2017YFE0106000), Ningbo Municipal Science and Technology Innovative Research Team (2015B11002 and 2016B10005), CAS Interdisciplinary Innovation Team, CAS Key Project of Frontier Science Research (QYZDBSSW-SYS030), Ningbo S&T Innovation 2025
References (45)
- et al.
Insertion of chlorine atoms onto π-bridges of conjugated polymer enables improved photovoltaic performance
Nanomater. Energy
(2019) - et al.
Synthesis and photovoltaic properties of small molecule electron acceptors with twin spiro-type core structure
Dyes Pigments
(2019) Organic photovoltaics: technology and market
Sol. Energy Mater. Sol. Cells
(2004)- et al.
Single-junction organic solar cell with over 15% efficiency using fused-ring acceptor with electron-deficient core
Joule
(2019) - et al.
ZnO nano-ridge structure and its application in inverted polymer solar cell
Org. Electron.
(2009) - et al.
Polymer photovoltaic cells: enhanced efficiencies via a network of internal donor-acceptor heterojunctions
Science
(1995) Two‐layer organic photovoltaic cell
Appl. Phys. Lett.
(1986)- et al.
Effect of LiF/metal electrodes on the performance of plastic solar cells
Appl. Phys. Lett.
(2002) - et al.
A wide band gap polymer with a deep highest occupied molecular orbital level enables 14.2% efficiency in polymer solar cells
J. Am. Chem. Soc.
(2018) - et al.
Organic and solution-processed tandem solar cells with 17.3% efficiency
Science
(2018)
Asymmetric fused-ring electron acceptor with two distinct terminal groups for efficient organic solar cells
J. Mater. Chem.
All-solution-Processed metal-oxide-free flexible organic solar cells with over 10% efficiency
Adv. Mater.
Aggregation and morphology control enables multiple cases of high-efficiency polymer solar cells
Nat. Commun.
All-polymer solar cells based on absorption-complementary polymer donor and acceptor with high power conversion efficiency of 8.27%
Adv. Mater.
Fullerene-free polymer solar cells with over 11% efficiency and excellent thermal stability
Adv. Mater.
13.34% efficiency nonfullerene all-small-molecule organic solar cells enabled by modulating crystallinity of donors via a fluorination strategy
Angew. Chem., Int. Ed. Engl.
Molecular optimization enables over 13% efficiency in organic solar cells
J. Am. Chem. Soc.
Modulation of end groups for low-bandgap nonfullerene acceptors enabling high-performance organic solar cells
Adv. Energy Mater.
A new nonfullerene acceptor with near infrared absorption for high performance ternary-blend organic solar cells with efficiency over 13
Adv. Sci.
Facile synthesis of polycyclic aromatic hydrocarbon (PAH)–Based acceptors with fine‐tuned optoelectronic properties: toward efficient additive‐free nonfullerene organic solar cells
Adv. Energy Mater.
16.67% rigid and 14.06% flexible organic solar cells enabled by ternary heterojunction strategy
Adv. Mater.
Enhanced power-conversion efficiency in polymer solar cells using an inverted device structure
Nat. Photon.
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