Guofang
Yang‡
ab,
Jing
Liu‡
a,
Lik-Kuen
Ma
a,
Shangshang
Chen
a,
Joshua Yuk Lin
Lai
a,
Wei
Ma
*b and
He
Yan
*ac
aDepartment of Chemistry and Energy Institute, The Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong, P. R. China. E-mail: hyan@ust.hk
bState Key Laboratory for Mechanical Behavior of Materials, Xi’an Jiaotong University, Xi’an 710049, P. R. China. E-mail: msewma@mail.xjtu.edu.cn
cThe Hong Kong University of Science and Technology-Shenzhen Research Institute, No. 9 Yuexing 1st RD, Hi-tech Park, Nanshan, Shenzhen 518057, China
First published on 11th May 2018
Carboxylate substitution is a common approach to tune the energy level of donor polymers for organic solar cells. However, the influence of carboxylate substitution on the morphological and electronic properties of donor polymers is not well understood. In this paper, we study two pairs of structurally similar terthiophene or quarterthiophene donor polymers with partial or complete carboxylate substitution on the alkyl side chains. It is found that the carboxylate substitution can enhance the crystallinity of the donor polymers and introduce larger and purer domains. Moreover, the polymers with the carboxylate substitution exhibit reduced bimolecular recombination due to the improved morphology. For device efficiencies, the terthiophene-based polymer, P3TEA (with 50% carboxylate substitution), exhibits the best performance. The alkyl side chains on P3TEA provide a typical temperature-dependent aggregation property, allowing for effective morphology control, while the carboxylate substitution deepens the HOMO level and enhances the crystallinity of the polymer. These benefits yield a near optimal morphology and high Voc value, and thus the best device efficiency among the polymers studied.
To develop efficient non-fullerene OSCs, it is not only important to synthesize high-performance non-fullerene acceptors, but also significant to design matching donor polymers to maximize the PCE of OSC devices. Several factors should be considered when designing a high-performance donor polymer. One is tuning the energy level to maximize the Voc and minimize the voltage loss.19–21 There are a variety of chemical strategies to tune the energy levels of OSC materials. Besides the commonly used fluorination strategy,22–26 another approach is to attach carboxylate groups,27,28 which is also electron withdrawing and thus can modulate the energy levels effectively. For example, a state-of-art donor polymer named P3TEA has been reported by partially attaching the carboxylate substitution on the alkyl side chains.19 This modification introduces an excellent device performance including a record-high Voc value of 1.11 V and a low voltage loss of 0.55 V. However, the influence of the carboxylate substitution on the morphological and electronic properties of the polymer is not well understood.
In this paper, we study two pairs of structurally similar terthiophene or quarterthiophene donor polymers with partial or complete carboxylate substitution on the alkyl side chains. It is found that carboxylate substitution can enhance the crystallinity of the donor polymers and introduce larger and purer domains. Moreover, light intensity dependent photocurrent measurement reveals that the polymers with the carboxylate substitution exhibit reduced bimolecular recombination due to the improved morphology. For device efficiencies, the terthiophene-based polymer, P3TEA (with 50% carboxylate substitution), exhibits the best performance. The alkyl side chains on P3TEA provide a typical temperature-dependent aggregation (TDA) property, allowing for effective morphology control, while the carboxylate substitution deepens the HOMO level and enhances the crystallinity of the polymer. These benefits yield a near optimal morphology and high Voc value, and thus the best device efficiency among the polymers studied.
Grazing incident wide angle X-ray scattering (GIWAXS) is utilized to characterize the molecular ordering of the polymers, with the profile shown in Fig. 2 and the 2D patterns displayed in the (ESI†). For the quarterthiophene system, it can be clearly seen that, in both pure and blend films, the q value of the (010) peak of P4TE is larger than that of P4TA, indicating a smaller d spacing value and closer π–π stacking. In the pure film, the π–π stacking d spacing value is 3.62 Å for P4TA, but 3.55 Å for P4TE. In the blend film, the π–π stacking d spacing of the P4TA polymer is estimated to be 3.59 Å, while that of the P4TE polymer is about 3.53 Å. In addition, the (010) peak of P4TE is sharper than that of P4TA, in both pure and blend film. As a result, P4TE has a larger coherence length (CL) than its analogues polymer P4TA. In the pure film, the CL is ∼47 Å for the P4TA polymer and ∼55 Å for the P4TE polymer. In the blend film, the CL of the P4TA polymer is estimated to be 37 Å, while that of the P4TE polymer is about 42 Å. These data all indicate that attaching the carboxylate substitution on the alkyl side chains can enhance the crystallinity of the polymer. For the terthiophene system, similar phenomenon was observed. In both pure and blend film, the q location of the (010) peak of P3TEA is larger than that of P3TA, showing that its d spacing is shorter and π–π stacking is closer. What's more, the (010) peak of P3TEA is sharper than that of P3TA, indicating that P3TEA has a longer CL. All the above results reveal that the carboxylated polymers have higher crystallinity in the terthiophene system, which is consistent with the conclusion in the quarterthiophene system.
Resonant soft X-ray scattering (R-SoXS) is a powerful tool for probing the in-plane composition of the blend films.31 A photon energy of 284.8 eV is selected for the R-SoXS measurement to maximize the contrast between the donor/accepter materials. The values of domain size and relative domain purity of the four blend films (listed in Table 1) are extracted from the R-SoXS profiles, as shown in Fig. 3. For the quarterthiophene system, the average domain size of the P4TA/SF-PDI2 blend film is about 15 nm, and the relative domain purity is a little low at ∼0.34. When it turns to the P4TE/SF-PDI2 blend film, the domain size is much larger at ∼44 nm, and the relative domain purity is also higher at ∼0.57. For the terthiophene system, similar trend was observed. Domain size of the P3TA/SF-PDI2 blend film is about 7.7 nm and its domain purity is about 0.64. Yet for its carboxylated counterpart P3TEA, domain size of the blend film is ∼13 nm and the relative domain purity is 1.00. What's more, AFM data (Fig. S5, ESI†) shows that the carboxylated polymers could have larger domains in the blend films. These results indicate that after attaching the carboxylate substitution on the alkyl side chains, the domains of the blend films are larger and purer.
q location (Å−1) | d spacing (Å) | Coherence length (Å) | Domain size (nm) | Domain purity (a.u.) | |
---|---|---|---|---|---|
P4TA pure | 1.7344 | 3.62 | 47.32 | N.A. | N.A. |
P4TE pure | 1.7668 | 3.55 | 55.16 | N.A. | N.A. |
P4TA/SF-PDI2 | 1.7483 | 3.59 | 36.99 | 15.15 | 0.3368 |
P4TE/SF-PDI2 | 1.7803 | 3.53 | 42.06 | 44.48 | 0.5699 |
P3TA pure | 1.6686 | 3.76 | 21.49 | N.A. | N.A. |
P3TEA pure | 1.7300 | 3.63 | 33.05 | N.A. | N.A. |
P3TA/SF-PDI2 | 1.6671 | 3.77 | 20.42 | 7.68 | 0.6369 |
P3TEA/SF-PDI2 | 1.7348 | 3.62 | 28.95 | 12.92 | 1.0000 |
Light intensity dependent photocurrent measurement was carried out for the four devices. The photocurrent follows a power-law dependence on light intensity, which can be described as Jph ∝ Pα (Jph = JL − JD, where JL and JD are the current density under illumination and in the dark, respectively). When the space charge buildup reaches fundamental limit, the power exponent α will equal to 0.75; while there is no space charge formed, α will equal to 1.32 Therefore, corresponding to the higher α value should be the less bimolecular recombination. The experimental power-law dependence of photocurrent on the incident light intensity was shown in Fig. 4. For the quarterthiophene system, α is 0.9611 in P4TA/SF-PDI2 based device, yet 0.9977 in the counterpart P4TE/SF-PDI2 based device. For the terthiophene system, the tendency was similar. The α value is 0.9831 in the P3TA/SF-PDI2 based device, while it turns to 0.9971 in the P3TEA/SF-PDI2 based device. These results indicate that attaching the carboxylate substitution on the alkyl side chains can reduce the bimolecular recombination within the PSC devices, which could be attributed to the improved morphology mentioned above.
Fig. 4 Experimental power-law dependence of photocurrent on the incident light intensity for the four devices. |
Blends | Hole mobility (cm2 V−1 s−1) | V oc (V) | J sc (mA cm−2) | FF | PCE (%) |
---|---|---|---|---|---|
a The values in parentheses stand for the average PCEs from over 20 devices. | |||||
P4TA/SF-PDI2 | 5.7 × 10−4 | 0.96 | 8.60 | 0.398 | 3.29 (3.00)a |
P4TE/SF-PDI2 | 7.0 × 10−4 | 1.06 | 9.27 | 0.541 | 5.34 (4.70)a |
P3TA/SF-PDI2 | 2.7 × 10−4 | 1.02 | 10.90 | 0.488 | 5.44 (4.45)a |
P3TEA/SF-PDI2 | 4.4 × 10−4 | 1.11 | 13.27 | 0.643 | 9.50 (8.63)a |
To better understand their morphology and device performance, TDA properties of the four polymers were tested, as shown in Fig. 5. For the quarterthiophene system, P4TA has an obvious TDA behavior as expected. The UV-Vis absorption spectra show a distinct red-shift when the temperature is lowered. Solution at 100 °C has an absorption maximum at ∼650 nm, while the solution at 20 °C is greatly red-shifted with a maximum at ∼770 nm. Moreover, at high temperatures, P4TA is well dissolved and disaggregated in solution. When the temperature is slowly reduced, a strong 0–0 transition peak at ∼700 nm gradually emerges. These phenomena reveal that P4TA has a typical TDA property. However, its analogues polymer P4TE does not own a notable TDA property. Obvious red-shift is not found when the solution temperature declines and even in low temperature as 20 °C, 0–0 transition peak is quite weak. Therefore, the ability of P4TE to control the morphology is poor, leading to excessively strong crystallinity, large domains (∼44 nm) and thus, low device performance. In the terthiophene system, obvious TDA behavior is found for the P3TA polymer. When the temperature falls, the red-shift of the UV-Vis absorption spectra is distinct and the absorption onset is markedly shifted from ∼650 nm at 100 °C to ∼770 nm at 20 °C. Interestingly, the counterpart polymer, P3TEA, keeps the TDA property. When the temperature decreases slowly, the red-shift of the absorption spectra is remarkable and the absorption maximum is greatly shifted from ∼650 nm at 100 °C to ∼770 nm at 20 °C. These phenomena reveal that the P3TEA polymer shows an obvious TDA behavior, and thus, an excellent ability of morphology control. What's more, the carboxylate substitution endows the P3TEA polymer an enhanced crystallinity compared with the counterpart polymer P3TA. Consequently, the P3TEA polymer owns a near-perfect morphology containing strong crystallinity, proper domain size and high domain purity. Combining its ultrahigh Voc value, it achieves the excellent device performance.
Fig. 5 Ultraviolet-Visible (UV-Vis) absorption spectra of the four polymer solutions (0.02 mg mL−1 in CB) at temperatures as indicated: (a) P4TA, (b) P4TE, (c) P3TA and (d) P3TEA. |
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8qm00101d |
‡ These authors contributed equally to this work. |
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