• Journal of Semiconductors
  • Vol. 43, Issue 5, 050501 (2022)
Ke Jin1, Zongliang Ou2, Lixiu Zhang1, Yongbo Yuan4..., Zuo Xiao1, Qiuling Song2, Chenyi Yi3 and Liming Ding1|Show fewer author(s)
Author Affiliations
  • 1Center for Excellence in Nanoscience (CAS), Key Laboratory of Nanosystem and Hierarchical Fabrication (CAS), National Center for Nanoscience and Technology, Beijing 100190, China
  • 2College of Materials Science & Engineering, Huaqiao University, Xiamen 361021, China
  • 3State Key Laboratory of Power System, Department of Electrical Engineering, Tsinghua University, Beijing 100084, China
  • 4School of Physics and Electronics, Central South University, Changsha 410083, China
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    DOI: 10.1088/1674-4926/43/5/050501 Cite this Article
    Ke Jin, Zongliang Ou, Lixiu Zhang, Yongbo Yuan, Zuo Xiao, Qiuling Song, Chenyi Yi, Liming Ding. A chlorinated lactone polymer donor featuring high performance and low cost[J]. Journal of Semiconductors, 2022, 43(5): 050501 Copy Citation Text show less

    Abstract

    Abstract

    The development of low-bandgap nonfullerene acceptors and wide-bandgap polymer donors speeds up the advance of organic solar cells (OSCs)[1-17]. Wide-bandgap copolymers based on fused-ring acceptor units are ideal donor materials due to their low-lying HOMO levels, high hole mobilities and complementary light absorption to nonfullerene acceptors[18-25]. Currently, high-performance donors with 18% power conversion efficiencies (PCEs) belong to this type. Fig. 1(a) summarizes these donors. They are D18-series copolymers based on dithieno[3',2':3,4;2'',3'':5,6]benzo[1,2-c][1,2,5]thiadiazole (DTBT) unit[15, 16, 26], PBQx-TF and PBQx-TCl based on dithieno[3,2-f:2',3'-h]quinoxaline (DTQx) unit[17, 25], and PM6 based on benzo[1,2-c:4,5-c']dithiophene-4,8-dione (BDD) unit[27]. However, the above building units require tedious synthetic routes, thus increasing the cost. Efficient yet low-cost copolymer donors are highly desired[13, 28, 29]. The fused-ring lactone unit, dithieno[3,2-b:2',3'-d]pyran-5-one (DTP), is a commercially available building block, which can be obtained via a few synthetic steps from cheap starting materials[30]. Previously, our group first reported lactone copolymer donors L1, L2 and L3 based on DTP unit[20, 31]. PCEs up to 17.81% was achieved from L3-based ternary solar cells, demonstrating the great potential of lactone copolymer donors. In this work, copolymerizing a cost-effective monomer (4,8-bis(4-chloro-5-(2-ethylhexyl)thiophen-2-yl)benzo[1,2-b:4,5-b']dithiophene-2,6-diyl)bis(trimethylstannane) (ClBDT-Sn)[32] with DTP monomer produced a new lactone copolymer L4. Ternary OSCs with L4 as the donor and N3[33] and PC61BM as the acceptors offered a PCE of 18.10% (certified 17.7%).

    (Color online) (a) Polymer donors offering PCEs over 18%. (b) J–V curves for L4:N3 and L4:N3:PC61BM solar cells. (c) EQE spectra for L4:N3 and L4:N3:PC61BM solar cells.

    Figure 1.(Color online) (a) Polymer donors offering PCEs over 18%. (b) JV curves for L4:N3 and L4:N3:PC61BM solar cells. (c) EQE spectra for L4:N3 and L4:N3:PC61BM solar cells.

    L4 was synthesized via Stille copolymerization and the details can be found in the Supporting Information. The number-average molecular weight (Mn) and polydispersity index (PDI) are 51.8 kDa and 1.58, respectively. The absorption spectra for L4 in chloroform and as a film are shown in Fig. S2. For film, L4 shows an absorption onset at 645 nm, corresponding to an optical bandgap of 1.92 eV. The light absorption of L4 is complementary to that of N3. Cyclic voltammetry (CV) measurements were employed to estimate the energy levels (Fig. S3). The highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) levels are –5.52 and –2.95 eV for L4, respectively.

    Solar cells with a structure of ITO/PEDOT:PSS/active layer/PDIN/Ag were made to assess the performance of L4. The D/A ratio, active layer thickness and diphenyl ether (DPE) additive content were optimized for L4:N3 cells (Tables S1–S3). The cells gave the highest PCE of 17.16%, with an open-circuit voltage (Voc) of 0.844 V, a short-circuit current density (Jsc) of 26.43 mA/cm2 and a fill factor (FF) of 76.9% (Fig. 1(b)). These cells have a D/A ratio of 1 : 1.4, an active layer thickness of 110 nm and 0.5 vol% DPE as the additive. Adding small amount of PC61BM into L4:N3 blend improved Voc, Jsc and FF simultaneously (Table S4). The L4:N3:PC61BM (1 : 1.4 : 0.2) ternary cells gave the highest PCE of 18.10%, with a Voc of 0.850 V, a Jsc of 27.07 mA/cm2 and an FF of 78.7%. The best ternary cells were also measured at the National Institute of Metrology (NIM), and a certified PCE of 17.7% (Voc, 0.856 V; Jsc, 26.43 mA/cm2; FF, 78.4%; effective area, 2.580 mm2) was recorded (Fig. S4). The external quantum efficiency (EQE) spectra indicate that after the addition of PC61BM, the EQE at 455–600 nm and 650–820 nm increased. The EQE maximum increased from 82% for binary cells to 88% for ternary cells (Fig. 1(c)). The integrated photocurrent densities are 25.13 and 26.13 mA/cm2, respectively, consisting with Jsc. The enhancement in Jsc and FF for ternary cells suggests the improved charge transport in the active layer. Hole and electron mobilities (μh andμe) were measured by using the space charge limited current (SCLC) method (Fig. S5 and S6)[34-42]. From binary to ternary blend films, μh increased from 7.91 × 10–4 to 9.23 × 10–4 cm2/(V·s), μe increased from 5.58 × 10–4 to 7.48 × 10–4 cm2/(V·s), and the μh/μe decreased from 1.42 to 1.23 (Table S5). The enhanced charge carrier mobilities and the more balanced charge transport benefit Jsc and FF for ternary cells. The active layer morphology was studied by using atomic force microscope (AFM) (Fig. S7). L4:N3:PC61BM (1 : 1.4 : 0.2) blend film is smoother than L4:N3 (1 : 1.4) film, as the root-mean-square roughnesses (Rrms) are 1.49 and 1.88 nm, respectively. Both blend films present typical nanofibers (diameter, ~20 nm) and fiber bundles.

    In short, by using a cost-effective lactone acceptor unit and a cost-effective chlorinated donor unit, we developed an efficient wide-bandgap polymer donor L4. L4 is a rare donor, featuring high performance (>18% PCE) and low cost. Lactone polymer donors hold promise for solar cells.

    Acknowledgements

    We thank the open research fund of Songshan Lake Materials Laboratory (2021SLABFK02), the National Key Research and Development Program of China (2017YFA0206600) and the National Natural Science Foundation of China (51773045, 21772030, 51922032 and 21961160720).

    Appendix A. Supplementary materials

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    Ke Jin, Zongliang Ou, Lixiu Zhang, Yongbo Yuan, Zuo Xiao, Qiuling Song, Chenyi Yi, Liming Ding. A chlorinated lactone polymer donor featuring high performance and low cost[J]. Journal of Semiconductors, 2022, 43(5): 050501
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