Lin Yang‡
a,
Daobin Yang‡ab,
Yao Chena,
Qian Luoa,
Mangang Zhanga,
Yan Huang*a,
Zhiyun Lu*a,
Hisahiro Sasabe*b and
Junji Kidob
aKey Laboratory of Green Chemistry and Technology (Ministry of Education), College of Chemistry, Sichuan University, Chengdu 610064, P. R. China. E-mail: huangyan@scu.edu.cn; luzhiyun@scu.edu.cn
bDepartment of Organic Device Engineering, Yamagata University, 4-3-16 Jonan, Yonezawa, Yamagata 992-8510, Japan. E-mail: h-sasabe@yz.yamagata-u.ac.jp
First published on 15th December 2015
Squaraines are promising donor materials because of their strong and broad absorption band in the visible and near infrared regions which is suitable for application in organic photovoltaic (OPV) cells. Two unsymmetrical squaraines (USQs), namely BIBISQ and TIBISQ, with two electron-donating aryls directly linked to the electron-withdrawing squaric acid core (Y-manner) can act as high performance donor materials for solution-processed bulk-heterojunction (BHJ) OPV cells. Both USQs show ideal low bandgaps (1.47 eV for BIBISQ and 1.39 eV for TIBISQ) with an intense and broad absorption band in the range of 500–900 nm, and relatively low HOMO levels of ∼−5.10 eV. The BHJ-OPV device based on both of them simultaneously showed excellent short current density (Jsc) (over 13 mA cm−2), open circuit voltage (Voc) (0.84 V), fill factor (FF) (0.49) and power conversion efficiency (PCE) of over 5% under a blend ratio of USQs
:
PC71BM = 1
:
3. These results indicate that the two USQs are quite promising candidates for small molecular (SM) OPV cells and the Y-manner should be a quite successful linking method for USQs.
:
0.8) when an oligothiophene derivative (DRCN5T) is employed as donor material.9
Recently, squaraines (SQs) have emerged as promising donor materials in OPVs due to their strong and broad absorption band in the visible and near infrared regions.10–16 Thus far, the record PCE of squaraine-based BHJ-OPV cells is 5.50% with a rather low donor content (D/A = 1
:
6)17 and the PCE of tandem devices based on squaraines is up to 8.3%.18
In recent years, our group has designed a series of unsymmetrical squaraines (USQs) in which the D and D′ segments are connected to the A subunit directly and via a methylidene bridge, respectively (X-manner in Scheme 1), and the PCE of these USQ-based BHJ-OPV devices is improved from 1.54% to 4.29%; however, the optimized D/A ratios fall into the region of 1
:
8–1
:
5 with a low donor content.19–22 According to the literature, the photophysical and chemical properties of squaraines are highly correlated with their linkage manner,23,24 which is closely related to their OPV performance. Therefore, very recently, our group has firstly designed some USQs with their two electron-donating aryls linked directly to the electron-withdrawing squaric acid core in Y-manner (Scheme 1).25 The OPV device based on them rendered a short current density (Jsc) of up to 12.03 mA cm−2 and a PCE of 4.35% with a D/A ratio of 1
:
5. These preliminary results indicated that D and D′ linked to A in Y-manner should be a quite promising linking manner for USQ donor materials. However, their PCE is unsatisfactory due to their relatively low open circuit voltage (Voc, 0.78 V) and fill factor (FF, 0.45). It is noteworthy that one of their donor segments is a pyrrole derivative, whose electron-donating ability is much better than phenyl groups, which leads to a relatively high HOMO energy level and then low Voc.
Therefore, from these previous results, two novel USQs with Y-manner linking have been designed and synthesized. Phenyl groups, such as N,N-dibutylaniline16,26 or 4-(p-tolyl)-1,2,3,3a,4,8b-hexahydrocyclopenta[b]indole, which are promising groups in OPV donor materials, were used as the D subunit;20,27 and 5-(8,9,10,10a-tetrahydrobenzo[e]cyclopenta[b]indol-7(7aH)-yl)benzene-1,3-diol was chosen as the D′ subunit.25 The molecular structures of two novel USQs (BIBISQ and TIBISQ) are shown in Scheme 2. Both show ideal low bandgaps of 1.47 eV for BIBISQ and 1.39 eV for TIBISQ with an intense and broad absorption band in the range 500–900 nm,28 and relatively low HOMO levels of ∼−5.10 eV. The BHJ-SMOPV cells based on both of them simultaneously showed enhanced Voc (0.84 V) and FF (0.49). Meanwhile, an excellent Jsc of over 13 mA cm−2 was achieved due to the relatively high content of USQs (USQs/PC71BM = 1
:
3). Ultimately, the PCEs of BHJ-SMOPV cells based on USQs were over 5%. In particular, the BHJ-SMOPV cell based on TIBISQ showed a high Jsc of up to 13.50 mA cm−2 and an excellent PCE of 5.49%, which could compare to the highest Jsc29 and PCE17,30,31 among all of the reported squaraine-based BHJ-OPV cells. These results indicate that Y-manner is indeed a quite promising linking method for the construction of high performance USQ-based OPV cells.
:
PC71BM (60 nm)/BCP (6 nm)/Al (100 nm). The patterned ITO-coated glass substrates were cleaned through sequential sonication in detergent, deionized water, acetone, and isopropanol for 20 min each. The cleaned substrates were dried in an oven at 65 °C for 12 h before use. The substrate was treated with UV-ozone for 30 min, then immediately transferred into a high vacuum chamber for deposition of 8 nm MoO3 at a pressure of less than 1 × 10−4 Pa with a rate of 0.2 Å s−1. Subsequently, the photoactive layer (thickness: 60 ± 5 nm) was fabricated by spin-casting a blend of the USQs and PC71BM in chloroform solution with a total concentration of 20 mg mL−1 (3500 rpm, 45 s) under a N2-filling glove box at 25 °C. Finally, the substrates were transferred back to the high-vacuum chamber, where BCP (6 nm) and Al (100 nm) were deposited as the top electrode at pressures of less than 2 × 10−4 Pa with a rate of 0.20 Å s−1 and 2.0–3.0 Å s−1, respectively. The active area of the OPV cells was 9 mm2. To obtain the average data related to device performance, several batches of devices (4 cells per batch) were fabricated and tested for each set of conditions. Current density–voltage (J–V) and external quantum efficiency (EQE) characterization of organic photovoltaic cells were performed on a CEP-2000 integrated system manufactured by Bunkoukeiki Co. The integration of EQE data over a AM 1.5G solar spectrum yielded calculated Jsc values with an experimental variation of less than 5% relative to Jsc measured under 100 mW cm−2 simulated AM 1.5G light illumination. Hole-only devices were fabricated with structures of ITO/MoO3 (8 nm)/USQs
:
PC71BM (60 nm)/MoO3 (8 nm)/Al (100 nm).
Samples for atomic force microscopy (AFM) measurements were prepared by spin-casting from USQs/PC71BM = 1
:
3 in chloroform solution on glass substrates.
:
1 v/v N,N-dimethylformamide (DMF)/N-methylpyrrolidinone (NMP) was heated at 120 °C for 12 h. The reaction mixture was then cooled to room temperature and filtered to remove the insoluble material. The precipitate was washed with ethyl acetate, and the combined filtrate was evaporated to dryness. Water was then added, and the aqueous phase was extracted with ethyl acetate. After silica gel column chromatography (hexane), a pale yellow oil (9.18 g, 85%) was obtained.
:
1) to give 5 (0.71 g, 30%) as a yellow solid. 1HNMR (400 MHz, CDCl3, ppm) δ 8.15 (d, J = 9.2 Hz, 2H, ArH), 6.75 (d, J = 9.2 Hz, 2H, ArH), 3.44 (t, J = 7.6 Hz, 4H, CH2), 1.69–1.61 (m, 4H, CH2), 1.46–1.37 (m, 4H, CH2), 1.03 (t, J = 7.2 Hz, 6H, CH3).
:
1) to give 6 (0.22 g, 25%) as an orange solid. 1HNMR (400 MHz, CDCl3, ppm) δ 8.01 (d, J = 8.4 Hz, 1H, ArH), 7.96 (s, 1H, ArH), 7.26–7.16 (m, 4H, ArH), 6.74 (d, J = 8.8 Hz, 1H, ArH), 4.99 (t, J = 8.4 Hz, 1H, CH), 3.89 (t, J = 8.4 Hz, 1H, CH), 2.38 (s, 3H, CH3), 2.14–2.01 (m, 1H, CH2), 1.92–1.85 (m, 2H, CH2), 1.76–1.66 (m, 2H, CH2), 1.56–1.44 (m, 1H, CH2).
:
9). Mp 219–221 °C. 1HNMR (400 MHz, CDCl3, ppm) δ 12.84 (s, 2H, OH), 8.15 (d, J = 8.8 Hz, 2H, ArH), 7.87 (d, J = 8.0 Hz, 1H, ArH), 7.83 (d, J = 8.4 Hz, 1H, ArH), 7.79 (d, J = 9.2 Hz, 1H, ArH), 7.71 (d, J = 8.8 Hz, 1H, ArH), 7.53 (t, J = 7.2 Hz, 1H, ArH), 7.44 (t, J = 7.2 Hz, 1H, ArH), 7.09 (s, 2H, ArH), 6.40 (s, 2H, ArH), 4.98–4.93 (m, 1H, CH), 4.39–4.34 (m, 1H, CH), 3.44 (t, J = 7.6 Hz, 4H, CH2), 2.39–2.25 (m, 2H, CH2), 2.12–1.99 (m, 2H, CH2), 1.79–1.67 (m, 4H, CH2), 1.58–1.49 (m, 2H, CH2), 1.44–1.35 (m, 4H, CH2), 0.99 (t, J = 7.2 Hz, 6H, CH3). 13CNMR (100 MHz, CDCl3, ppm) δ 182.8, 178.1, 166.5, 164.6, 155.2, 152.6, 140.1, 132.5, 130.9, 130.7, 130.1, 128.8, 128.6, 126.9, 124.5, 123.3, 117.8, 115.2, 112.3, 108.0, 97.0, 69.7, 51.2, 44.7, 35.1, 33.3, 29.6, 24.8, 20.2, 13.9. HRMS (ESI)+ m/z: [M + H]+ calcd for C39H41N2O4, 601.3061; found, 601.3062. Anal. calcd for C39H40N2O4: C, 77.97; H, 6.71; N, 4.66. Found: C, 78.11; H, 6.94; N, 5.12.
:
9). Mp 248–249 °C. 1HNMR (400 MHz, CDCl3, ppm) δ 12.69 (s, 2H, OH), 8.02 (d, J = 8.4 Hz, 1H, ArH), 7.97 (s, 1H, ArH), 7.84 (d, J = 8.4 Hz, 1H, ArH), 7.79 (d, J = 8.4 Hz, 1H, ArH), 7.75 (d, J = 8.8 Hz, 1H, ArH), 7.69 (d, J = 8.8 Hz, 1H, ArH), 7.52 (t, J = 7.2 Hz, 1H, ArH), 7.40 (t, J = 7.2 Hz, 1H, ArH), 7.26 (d, J = 8.0 Hz, 2H, ArH), 7.20 (d, J = 8.4 Hz, 2H, ArH), 6.75 (d, J = 8.0 Hz, 1H, ArH), 6.38 (s, 2H, ArH), 4.98 (s, 1H, CH), 4.91 (s, 1H, CH), 4.32 (s, 1H, CH), 3.85 (s, 1H, CH), 2.39 (s, 3H, CH3), 2.36–2.19 (m, 2H, CH2), 2.12–1.84 (m, 5H, CH2), 1.77–1.66 (m, 3H, CH2), 1.57–1.45 (m, 2H, CH2). 13CNMR (100 MHz, CDCl3, ppm) δ 182.9, 177.6, 165.8, 164.5, 155.1, 154.5, 140.1, 136.9, 136.8, 135.7, 133.1, 130.9, 130.8, 130.3, 130.1, 128.8, 128.6, 126.9, 126.2, 124.5, 123.3, 123.2, 120.6, 115.2, 108.1, 108.0, 97.0, 70.9, 69.7, 44.7, 44.4, 35.5, 35.1, 33.3, 32.8, 24.8, 24.0, 21.1. HRMS (ESI)+ m/z: [M + H]+ calcd for C43H37N2O4, 645.2748; found, 645.2748. Anal. calcd for C43H36N2O4: C, 80.10; H, 5.63; N, 4.34. Found: C, 80.52; H, 5.74; N, 4.82.| Compound | λabsa (nm) (log ε) |
λabsb (nm) | FWHM (nm) | Eoptg (eV) | Eox (V) | HOMOc (eV) | LUMOd (eV) | |
|---|---|---|---|---|---|---|---|---|
| Solution | Film | |||||||
| a Measured in dilute chloroform solution (5.00 × 10−6 M).b Measured in thin film state.c HOMO= (−4.80 − Eox) eV.d LUMO = Eoptg + HOMO. | ||||||||
| BIBISQ | 691 (5.32) | 748 | 53 | 184 | 1.47 | 0.32 | −5.12 | −3.65 |
| TIBISQ | 713 (5.50) | 760 | 61 | 217 | 1.39 | 0.28 | −5.08 | −3.69 |
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| Fig. 2 Cyclic voltammograms of the two USQs (a) and the energy levels of the components for OPV devices (b). | ||
:
PC71BM (60 nm)/BCP (6 nm)/Al (100 nm). The corresponding data and curves are shown in Table 2, Fig. 3 and 4. The results indicated that a similar trend in photovoltaic performance of OPV devices based on both BIBISQ and TIBISQ could be observed when their D/A ratio was varied from 1
:
1 to 1
:
8. Taking TIBISQ as an example, when the blend ratio was changed from 1
:
1 to 1
:
8, the Voc and FF values of the corresponding BHJ-OPV devices were almost unaltered, while Jsc showed a distinct variation, which matched with the corresponding EQE spectra of the devices. As shown in Fig. 3b, three major bands could be identified in the EQE spectra of TIBISQ devices, with their peaks approximately located at 380 nm, 480 nm and 760 nm, respectively. The first two high-energy bands should stem from the absorption of PC71BM, and the third low-energy band at ∼760 nm should arise from the absorption of TIBISQ. With increasing composition of TIBISQ, the intensity of the third band peaked at ∼760 nm increased gradually, which is consistent with the corresponding absorption spectrum of D/A blend film with a similar D/A mixing ratio (shown in Fig. 3c). Accordingly, with increasing D/A ratio from 1
:
8 to 1
:
3, Jsc of the TIBISQ device increased gradually from 10.92 to 13.02 mA cm−2. However, in the case of the TIBISQ device with a D/A ratio of 1
:
1, the intensity of the third band in its EQE spectrum decreased drastically rather than increasing, despite the fact that the 1
:
1 blend film displayed the strongest absorption in this band, as shown in Fig. 3c. This may be ascribed to the drastically different morphology of the blend films between 1
:
1 and other D/A ratios (Fig. 5). Similarly, for BIBISQ devices, the optimum D/A ratio was also found to be 1
:
3. Therefore, taking advantage of the more effective absorption in the NIR region due to the increased content of USQ in the 1
:
3 optoelectronic film, the resulting devices both showed impressive Jsc values of ∼13 mA cm−2, which is much higher than that of the reported USQ-based BHJ-SMOPV devices.15,25 Additionally, according to the experimental and calculated results (Fig. 6), the hole mobility of the as-prepared 1
:
3 D/A blending films was relatively high (3.25 × 10−5 and 6.21 × 10−5 cm2 V−1 s−1 for BIBISQ- and TIBISQ-based film in sequence), which would also contribute to the high Jsc and FF,36 hence the high PCE of 4.97–5.08% of the devices.
| Active layer (w/w) | Voc (V) | Jsc (mA cm−2) | FF | PCEb (%) |
|---|---|---|---|---|
| a Thermally annealed at 80 °C for 10 min.b The average PCE values are shown in parentheses. | ||||
TIBISQ : PC71BM = 1 : 1 |
0.83 | 9.95 | 0.45 | 3.72 (3.65) |
TIBISQ : PC71BM = 1 : 3 |
0.83 | 13.02 | 0.47 | 5.08 (5.03) |
TIBISQ : PC71BM = 1 : 5 |
0.84 | 11.15 | 0.50 | 4.68 (4.57) |
TIBISQ : PC71BM = 1 : 8 |
0.84 | 10.92 | 0.48 | 4.40 (4.32) |
TIBISQ : PC71BM = 1 : 3a |
0.83 | 13.50 | 0.49 | 5.49 (5.39) |
BIBISQ : PC71BM = 1 : 1 |
0.83 | 8.23 | 0.43 | 2.94 (2.81) |
BIBISQ : PC71BM = 1 : 3 |
0.84 | 12.87 | 0.46 | 4.97 (4.92) |
BIBISQ : PC71BM = 1 : 5 |
0.85 | 10.97 | 0.49 | 4.57 (4.46) |
BIBISQ : PC71BM = 1 : 8 |
0.86 | 10.41 | 0.47 | 4.21 (4.13) |
BIBISQ : PC71BM = 1 : 3a |
0.83 | 13.13 | 0.49 | 5.34 (5.24) |
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| Fig. 3 The J–V characteristics (a); and EQE characteristics (b) of the TIBISQ devices; and absorption spectra (c) of the photoactive layers with different D/A ratios. | ||
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| Fig. 4 The J–V characteristics (a); and EQE characteristics (b) of the BIBISQ devices; and absorption spectra (c) of the photoactive layers with different D/A ratios. | ||
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Fig. 5 Tapping-mode AFM height images (5 × 5 µm) of TIBISQ : PC71BM blend films with different blend ratios ((a) 1 : 1; (b) 1 : 3). | ||
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Fig. 6 Current density–voltage characteristics of hole-only single-carrier devices using USQs : PC71BM = 1 : 3 blend films as active layer. | ||
Upon thermal annealing (80 °C, 10 min), the device performance of both BIBISQ and TIBISQ was enhanced, with PCE values of 5.34% and 5.49%, respectively. The enhanced PCEs are attributed not only to the improved Jsc (for BIBISQ, from 12.87 to 13.13 mA cm−2; for TIBISQ, from 13.02 to 13.50 mA cm−2), which is consistent with their EQE measurement results (shown in Fig. 3b and 4b), but also to the enhanced FF (for BIBISQ, from 0.46 to 0.49; for TIBISQ, from 0.47 to 0.49). Moreover, the impressive Jsc (13.50 mA cm−2) and excellent PCE (5.49%) of TIBISQ-based BHJ-OPV are among the highest Jsc29 and PCE17,30,31 values of all of the reported squaraine-based BHJ-OPV cells. These results indicate that the Y-mannered molecular backbone is indeed quite promising for the construction of successful OPV USQs with increased donor content in the photoactive layer.
It is worth mentioning that the optimized D/A composite ratio in these devices based on two USQs is 1
:
3. Generally, a larger content of donor material in the blend film is propitious to the harvesting of sunlight, hence the enhancement of PCE of the device,37 therefore, the typical D/A ratio in highly efficient OPV devices lies in the range of 1
:
1–1
:
2.9 However, although many D/A composite ratios have been employed in BHJ-OPV devices based on squaraines, the record PCE of 5.50% for BHJ-OPV devices using symmetrical squaraines (SSQs, D–A–D-type) was achieved with a rather low D/A ratio (1
:
6), according to Wei's report.17 Similarly, for our reported USQ donor materials, the optimized D/A ratios fell in the region 1
:
8–1
:
5.19–22 The low content of donor material in the photoactive layer may hamper the photovoltaic performance of these squaraine materials. Therefore, the present investigation shows that a much enhanced content of USQ donor materials in the active layers (the optimized D/A ratios of BHJ-OPV cells based on BIBISQ and TIBISQ are both 1
:
3) is beneficial to absorb more solar light in the NIR region, which contributes to the impressive Jsc over 13 mA cm−2 and PCE over 5% of BHJ-OPV devices, which would open a more promising route to improve the OPV performance of squaraine materials by molecular tailoring.
:
3). Consequently, Y-manner is indeed a quite promising linking method for the construction of high performance OPV USQs in terms of increased donor content.
Footnotes |
| † Electronic supplementary information (ESI) available: The 1H NMR, 13C NMR and HRMS spectra of BIBISQ and TIBISQ. See DOI: 10.1039/c5ra24186c |
| ‡ The first two authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2016 |