Open Access Article
:
4,5-b′]difurans as donor building blocks for the formation of novel donor–acceptor copolymers†
Carmen L.
Gott-Betts
,
Alfred A.
Burney-Allen
,
David L.
Wheeler
and
Malika
Jeffries-EL
*
Department of Chemistry, Division of Materials Science and Engineering, Boston University, Boston, MA 02115, USA. E-mail: malikaj@bu.edu
First published on 12th May 2022
Four donor–acceptor copolymers combining the novel electron-donating moiety, 2,3,6,7-tetra(thiophen-2-yl)benzo[1,2-b
:
4,5-b′]difuran (BDF) with either 2,3,1-benzothiadiazole (BT) or 2-octyl-2H-benzo[d][1,2,3]triazole (BTz) as the electron-accepting unit were prepared via the Stille cross-coupling reaction. Two different alkyl chains were attached on the BDF monomers and the impact on the polymers’ solubility and thin film morphology was evaluated. The resulting polymers had optical bandgaps between 1.7–1.9 eV and HOMO levels that ranged from −5.60 to −5.85 eV. In thin films, the BTz copolymer showed absorption bands in the range of 400–625 nm. The BT copolymer exhibited two absorption bands: one from 350–450 nm and a broad absorption in the range of 450–750 nm. When the polymers were used as donor materials with the electron-acceptor PC71BM in bulk-heterojunction photovoltaic cells, power conversion efficiencies of up to 2.93% were obtained. These results indicate that BDF is a promising building block for the synthesis of donor materials for use in organic solar cells, due to the favorable energy levels. Although, additional modifications are needed to improve device performance.
The benzo[1,2-b
:
4,5-b′]dithiophene (BDT) moiety has been comprehensively investigated as the electron-donating species in donor–acceptor (D/A) conjugated polymers.13–16 BDT has a planar backbone that facilitates pi-stacking and enhances charge carrier mobilities. As a result, BDT-based organic semiconductors are among the highest performing materials in the field of OPVs with photocurrent efficiencies (PCE) of ∼16.0%,17,18 and hole mobilities exceeding 0.1
cm2
V−1 s−1.19 Due to the success of BDT-based materials in these applications, our group has turned its focus towards the development its oxygen containing analog, benzo[1,2-b
:
4,5-b′]difuran (BDF). Furan is isoelectronic to thiophene, but oxygen has a smaller atomic radius than sulfur. Thus, the steric hindrance between adjacent heterocycles is reduced and the planarity between adjacent rings is increased.20,21 At the same time, BDF-based materials have been shown to exhibit improved solubility compared to their BDT analogs.20,22 Furthermore, the lower Dewar resonance energy of furan relative to thiophene makes the formation of quinoidal structures more favorable.23 Consequently, BDF containing materials have a narrower bandgap and more stabilized HOMO level in comparison to their BDT analogs.24–26
Previously we published the synthesis of a new BDF-based building block, 5,5′-(3,7-didecylbenzo[1,2-b
:
4,5-b′]difuran-2,6-diyl)bis(4-alkylthiophene-5,2-diyl)bis(trimethyl-stannane) and utilized it in D–A copolymers with 6,6′-dibromo-N,N′-(2-octyldodecanyl)-isoindigo.27 The resulting polymers exhibited two main absorption bands: a high energy band due to the π–π* transition, and a low energy band due to intramolecular charge transfer between the donor and acceptor units. However, the poor solubility of the copolymer adversely impacted the film morphology. As a result, the OPVs fabricated from these polymers exhibited low PCEs of ∼1.0%. In another report, we detailed the copolymerization of BDF with the electron deficient 1,4-diketopyrrolo[3,4-c]pyrrole (DPP) moiety.28 Although the absorption profile was strong and broad within the 600–800 nm range, like many DPP containing polymers, these materials also had poor solubility. As a result of the film morphology, modest device performances of ∼3.0% were attained.
In this report, to further improve upon our BDF building block we introduced thienyl substituents onto the BDF moiety. Using aromatic substituents instead of alkyl or alkoxy-chains broadens absorption profiles and improves the intramolecular charge transfer (ICT) within the material.24 Our functional BDF has reactive handles at the 3- and 7-positions. Thus, this molecule can be used to produce novel two-dimensional BDF monomers as most of the previous examples of two-dimensional BDT/BDF polymers have the aryl substituents at the 4- and 8-positions.19,22,29 Herein, We synthesized four donor–acceptor copolymers using a novel two-dimensional monomer 2,3,6,7-tetra(thiophen-2-yl)benzo[1,2-b
:
4,5-b′]difuran with either 2,3,1benzothiadiazole (BT) or 2-octyl-2H-benzo[d][1,2,3]triazole (BTz) as the comonomer. Here, BT and BTz were chosen for their facile synthesis and their demonstrated utility in high performing OPV materials.23,24 For the two-dimensional axillary thiophenes, alkyl side chains were attached to enhance solubility. The alkyl chain length was also varied to evaluate its impact on device performance.
The synthesis for the polymers is shown in Scheme 2. The polymers were all synthesized via Stille cross-coupling reaction of either 8a or 8b with the corresponding comonomers to yield polymers P1–P4. The yields ranged from 51–84% after purification via Sohxlet extraction. All polymers were soluble in chloroform at room temperature enabling characterization by proton nuclear magnetic resonance spectroscopy (1H NMR).
The spectra obtained are consistent with the expected polymer structures. The molecular weights were assessed using gel permeation chromatography (GPC) at 25 °C using THF as the eluent. The resulting characterization data is summarized in Table 1. Comparing the molecular weights of polymers with the same alkyl chain (P1vs.P2, P3vs.P4), P2 has a slightly lower molecular weight (Mn and Mw) when compared to its BTz analog P1. Further, both polymers have low degrees of polymerization, indicating that the ethyl hexyl side chain is not adequate to impart solubility. Conversely, P3 has a lower molecular weight compared to P4. Assuming equal reactivity, this suggests that the additional alkyl chain on the BTz unit did not increase the solubility of the polymer. When comparing the polymers with the same acceptor units (P1vs.P3, P2vs.P4), the 2-ethylhexyl substituted polymers have lower molecular weights and degrees of polymerization than the 2-octyldodecyl variants. Assuming equal reactivity, this suggests that the longer branched alkyl substituents on the BDF core are better for improving solubility and increasing molecular weight.
| Polymer | Yielda (%) | M n (Da) | M w (Da) | Đ | DPn | T d (°C) |
|---|---|---|---|---|---|---|
| a Isolated yield after Soxhlet extraction. b Molecular weight data was obtained by GPC (see ESI). c 5% weight loss temperature determined by TGA. | ||||||
| P1 | 65 | 6155 | 9045 | 1.47 | 10 | 393 |
| P2 | 84 | 4898 | 6246 | 1.28 | 7 | 363 |
| P3 | 76 | 11 453 |
17 305 |
1.51 | 14 | 379 |
| P4 | 51 | 20 054 |
29 558 |
1.47 | 26 | 389 |
The thermal properties of the polymers were evaluated using differential scanning calorimetry (DSC) and thermal gravimetric analysis (TGA). DSC did not reveal any observable phase transitions for temperatures up to 250 °C. The TGA results are summarized in Table 1 and indicate that 5% weight loss onsets occurred between 363–393 °C. This thermal data supports that these polymer materials are thermally stable well above the operating temperature threshold for organic photovoltaic devices.32
nm respectively. Whereas the spectra for the BT polymers P2 and P4 have two distinct absorption bands as is typically seen in D/A copolymers: a low energy peak resulting from intramolecular charge transfer (ICT) and a higher energy peak associated with the π–π* transition.33 In the solid-state spectra, the small high energy bands for P1 and P3 have almost disappeared, and the lower energy peaks now display small shoulders, slightly broadened peak widths, and concurrent red-shifting of the λmax. The side chains did not have any impact on the solid-state packing as the λmax for both P1 and P3 shifted by 26 nm from solution to film. Conversely, the spectra for the BT polymers showed a significant peak broadening between the solution and solid state along with a hypsochromic shift of all peaks. The extent of spectral broadening and shifting was dependent on the length of the side chains, with P4 being the broadest.
| Polymer | λ max (nm) Solution | λ max (nm) Film |
E
OPTg a (eV) |
HOMOb (eV) | LUMOc (eV) |
|---|---|---|---|---|---|
| a Optical bandgap as measured by the optical onset (Eg = 1240/λoffset). b HOMO levels measured by CV (see ESI). c Estimated LUMO = HOMO+Eg. | |||||
| P1 | 513 | 539 | 1.9 | −5.85 | −4.0 |
| P2 | 403, 545 | 421, 585 | 1.7 | −5.60 | −3.9 |
| P3 | 520 | 546 | 1.9 | −5.71 | −3.8 |
| P4 | 417, 592 | 437, 622 | 1.7 | −5.82 | −4.1 |
To evaluate the electrochemical properties of the polymers, the redox profile was evaluated using cyclic voltammetry, see ESI.† All four polymers exhibit measurable and reproducible oxidation processes, but reduction curves were not observed. The HOMO levels were estimated from the onset of oxidation using the absolute energy level of ferrocene/ferrocenium (Fc/Fc+) as 5.1 eV under vacuum and are summarized in Table 2. The polymers had calculated HOMO values between −5.60 eV and −5.85 eV affording good stability in air, and open circuit voltage (VOC), making them suitable for use in OPVs.34 The LUMO values were estimated from the HOMO and the optical bandgap and ranged from −3.8 eV to −4.1 eV. As a result, the offset between the polymer LUMO and that of the fullerene (−4.1 eV) acceptor is small, which can negatively impact device performance.35
| Polymer | Additive (%) | J SC (mA cm−2) | V OC (V) | FF | PCE (%) | RMS |
|---|---|---|---|---|---|---|
| Average of 8 devices. | ||||||
| P1 | None | 8.47 ± 0.40 | 0.50 ± 0.01 | 34.77 ± 1.31 | 1.67 ± 0.10 | — |
| 2% CN | 8.80 ± 0.79 | 0.60 ± 0.01 | 37.19 ± 1.03 | 1.98 ± 0.21 | 0.512 | |
| P2 | None | 6.69 ± 0.33 | 0.64 ± 0.02 | 35.10 ± 0.79 | 1.51 ± 0.09 | — |
| 1% CN | 6.99 ± 0.52 | 0.64 ± 0.4 | 33.62 ± 1.15 | 1.53 ± 0.15 | 0.558 | |
| P3 | None | 4.60 ± 0.19 | 0.81 ± 0.00 | 58.89 ± 1.10 | 2.22 ± 0.08 | — |
| 1% CN | 5.21 ± 0.27 | 0.83 ± 0.00 | 56.15 ± 1.05 | 2.45 ± 0.15 | 9.916 | |
| P4 | None | 5.79 ± 0.34 | 0.72 ± 0.01 | 65.36 ± 0.90 | 2.75 ± 0.15 | 0.739 |
| 1% CN | 5.47 ± 0.40 | 0.73 ± 0.00 | 57.90 ± 2.35 | 2.33 ± 0.18 | — | |
Among the devices fabricated without solvent additives, P4 gave the highest PCE at 2.93% with the highest FF of 64.86. P4 also demonstrated a moderate VOC of 0.73 V and moderate JSC of 6.18 mA cm−2. P1 and P2 gave lower efficiencies at 1.81% and 1.63% respectively. The lowest performing polymer, P2, had a modest VOC at 0.67 V but a lower FF of 35.07 and JSC of 6.93 mA cm−2. When CN was added, there was an increase in performance for all the polymers except for P4, due to increases in JSC and/or VOC. P3 had the highest performing device at 2.67% under these conditions. The highest performing device for P1 required a 2% CN additive compared to 1% for the other three polymers. The decrease in the P4 device performance with the addition of CN additive is likely a result of its higher solubility than the other polymers.
A comparison of the alkyl chains shows that the ethylhexyl polymers P1 and P2 had significantly lower FF than their octyldodecyl variants, P3 and P4. Conversely, P1 and P2 showed higher JSC compared to the octyldodecyl polymers, P3 and P4. Overall polymers with ethylhexyl side chains had poorer performance when compared to their octyldodecyl counterparts. Next, when comparing polymers with different electron withdrawing units, the nature of the electron deficient comonomer was not significant as P1 performed better than P2, but P4 performed better than P3.
To further investigate the performance trends, the morphology of the highest performing polymer/PC71BM devices was evaluated using atomic force microscopy (AFM) as shown in Fig. 3. The root mean-square (RMS) values are shown in Table 3. When first evaluating the effect of alkyl chain length on the BDF donor, it was observed that P2 and P4 formed relatively smooth films with RMS roughness values of 0.56 and 0.74. The OPV performance increased from 1.75% for P2 to 2.93% with P4 even though P4 had a higher roughness value. Analogously, P1 has a very smooth film compared to P3 with RMS values of 0.51 and 9.9, respectively. Although P3 has a very large RMS value, the overall device performance was like P1 with PCE values of 2.67% and 2.33% respectively. While it has been reported that a higher RMS value may lead to better photovoltaic performance,36 high RMS values indicate that the device films made with P3 have pinholes and/or completely void areas. In comparing the electron accepting unit within the D–A polymer it was observed that P1 and P2 have similar RMS values of 0.51 and 0.56 respectively. Thus, the heterocycles have less of an impact on film morphology than the side chains do. Whereas, for P3 and P4, the RMS values were too different to determine if the difference in performance was due to the smoother film or to the intrinsic optical properties of the materials. However, it is impressive that P3 has such a high PCE considering the severe film defects. These results suggest that a mid-range side chain may be beneficial to improve device properties. Further optimization of the P3 device film would be necessary to produce truly optimized devices.
:
4,5-b′]difurans bearing different alkyl chains were synthesized. Polymer pairings with the same comonomer had similar absorption profiles and optical bandgaps, regardless of the side-chain length. Whereas the polymer sets with the same alkyl chain had different optical profiles due to the relative difference in the strength of the electron acceptor unit. It was hypothesized that the two-dimensional BDF monomer would lead to improvements in OPV performance. The resulting polymers had low-lying LUMO levels, and deep HOMO-levels both of which were favorable for a novel OPV donor materials. However, the band gaps ranging from 1.7–1.9 eV, which combined with the poor film forming properties lead to modest OPV performances. Despite these outcomes, the aforementioned synthetic ease and oxidative stability make the BDT moiety a promising building block for designing new materials.37 In the future, we will investigate the BDF moiety with stronger electron-accepting comonomers. Doing this would both reduce the polymer bandgap and allow for the use of additional alkyl character to improve solubility and improve film formation.
:
2–3 and 1
:
1 blend ratio (20 mg mL−1), respectively, with chlorobenzene as the processing solvent. The prepared solutions were allowed to stir for 24 h at 80 °C prior to spin coating onto the PEDOT:PSS layer at 1000 rpm for 2 minutes. Following spin coating, Calcium (15 nm) and Aluminum (100 nm) electrodes underwent successful deposition via thermal evaporation. Films were also evaluated under post thermal annealing conditions at 100 °C for 10 minutes. Current–density (J–V) data were obtained via Keithley 2400 source meter and simulated AM 1.5 G illumination (100 mW cm−2, Newport 91160) calibrated using a KG-5 filter Silicon reference cell.
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1) and 2-iodothiophene (7.10 mL, 64.27 mmol) then stirred overnight at room temperature. The reaction mixture was poured into ice and extracted three times with dichloromethane. The combined organic layers were washed with saturated aqueous NH4Cl, water, and brine. The organic layer was dried over MgSO4, evaporated, and purified using a silica plug (hex/DCM 4
:
1). The resulting solid was recrystallized from ethyl acetate/hexanes (2
:
1) to yield 2 as a yellow solid (8.09 g, 79% yield). 1H NMR (500 MHz, CDCl3) δ 7.31 (m, 4H), 7.02 (m, 4H), 3.90 (s, 6H). 13C NMR (125 MHz, CDCl3) δ 153.87, 132.37, 127.75, 127.27, 123.28, 115.44, 113.28, 89.47, 88.40, 77.41, 77.16, 76.91, 56.58. LRMS (ESI) m/z: [M+H]+ calculated for C20H14O2S2
:
350.04; found: 351.0513 m/z, error 1.0113 ppm.
:
1) (5.68 g, 70% yield). 1H NMR (500 MHz, CDCl3) δ 7.39 (d, J = 3.53 Hz, 2H), δ 7.15 (d, J = 3.5 Hz, 2H), δ 6.99 (s, 2H), δ 3.88 (s, 6H), δ 1.34 (m, 6H), 1.11 (d, J= 7.44 Hz, 36H). 13C NMR (125 MHz, CDCl3) δ 153.57, 138.10, 135.28, 132.75, 127.74, 115.13, 113.13, 90.41, 88.22, 77.16, 76.91, 76.65, 56.33, 18.41, 11.65. HRMS (ESI) m/z: [M+H]+ calculated for C38H54O2S2Si2
:
663.3182; found: 663.3209 m/z, error 4.0704 ppm.
:
4,5-b′]difuran-2,6-diyl)bis(thiophene-5,2-diyl))bis(triisopropylsilane) (4).
A 500 mL Erlenmeyer flask was charged with 3 (5.30 g, 8 mmol) which was dissolved in CH2Cl2 and cooled to 0 °C. The solution was rapidly stirred as iodine (6.09 g, 23.98 mmol) in 200 mL CH2Cl2/hexanes (3
:
1) was added dropwise over 10 minutes. Upon completion of the addition, the reaction mixture was stirred at 0 °C for 4 hours. The cold reaction mixture was then filtered to collect the crude product. The solid was stirred in hot hexanes, cooled, and filtered. The yellow solid was then recrystallized from toluene to afford yellow crystals (5.18 g, 73% yield). 1H NMR (500 MHz, CDCl3) δ 8.08 (d, J = 3.6 Hz, 2H), δ 7.45 (s, 2H), δ 7.33 (d, J = 3.6 Hz, 2H), δ 1.40 (m, 6H), 1.15 (d, J = 7.4 Hz, 36H). HRMS (ESI) m/z: [M+H]+ calculated for C36H48I2O2S2Si2
:
886.07; found: 887.0829, error 3.0437 ppm.
:
1) under nitrogen. The reaction mixture was heated at 80 °C overnight. Next, the mixture was poured into 100 mL of water and extracted three times with dichloromethane. The combined organic layers were washed with deionized water, NH4Cl, brine, and dried over MgSO4. The solvent was removed in vacuo and the residue was sent through a silica plug using hexanes then used without further purification as a viscous, orange semi-solid. (6a, 86%): 1H NMR (500 MHz, CDCl3) δ 7.60 (s, 2H), δ 7.57 (d, J = 3.60 Hz, 2H), δ 7.17 (d, J = 3.61 Hz, 2H), δ 7.12 (d, J = 3.40 Hz, 2H), δ 6.86 (d, J = 3.39 Hz, 2H), δ 2.85 (d, J = 6.69 Hz, 4H), δ 1.67 (m, 2H), δ 1.30–1.45 (m, 22H), δ 1.11 (d, J = 7.4 Hz, 36H), δ 0.95 (m, 12H). HRMS (ESI) m/z: [M+H]+ calculated for C60H86O2S4Si2
:
1022.50; found: 1023.5139, error 1.0747 ppm. (6b, 81%): 1H NMR (400 MHz, CDCl3) δ 7.60 (s, 2H), 7.56 (d, J = 3.6 Hz, 2H), 7.17 (d, J = 3.7 Hz, 2H), 7.12 (d, J = 3.3 Hz, 2H), 6.85 (d, J = 3.3 Hz, 2H), 2.85 (d, J = 6.6 Hz, 4H), 1.71 (m, 2H), 1.36 (m, 70H), 1.11 (d, J = 7.3 Hz, 36H), 0.89 (m, 12H).
:
710.24; found:: 711.2477, error 2.5308 ppm. (7b, 93%): 1H NMR (500 MHz, CDCl3) δ 7.58 (d, J = 0.6 Hz, 2H), 7.51 (d, J = 3.7 Hz, 2H), 7.30 (d, J = 6.1 Hz, 2H), 7.11 (d, J = 3.4 Hz, 2H), 7.07–7.00 (m, 2H), 6.86 (d, J = 3.4 Hz, 2H), 2.85 (d, J = 6.7 Hz, 4H), 1.74–1.69 (m, 2H), 1.36–1.21 (m, 64H), 0.88 (d, J = 5.1 Hz, 12H). 13C NMR (125 MHz, CDCl3) δ 151.20, 148.68, 146.51, 132.61, 129.59, 129.36, 128.24, 127.50, 126.64, 110.83, 40.25, 34.93, 33.51, 32.08, 31.75, 30.19, 29.87, 29.53, 26.84, 25.44, 22.85, 14.27. HRMS (ESI) m/z: [M+H]+ calculated for C66H94O2S4
:
1046.61; found: 1047.6223, error 0.7636 ppm.
:
1H NMR (500 MHz, CDCl3) δ 8.04 (br, 2H), δ 7.82 (br, 1H), δ 7.45 (br, 4H), δ 7.12 (br, 2H), δ 6.88 (br, 2H), δ 6.78 (br, 1H), δ 4.79 (br, 2H), δ 2.74–2.90 (br, 4H), δ 2.20 (br, 2H), δ 1.28–1.71 (br, 28H), δ 0.87–0.98 (br, 15H). P3
:
1H NMR (500 MHz, CDCl3, δ) 8.08 (br, 2H), 7.84 (br, 1H), 7.58 (br, 2H), 7.43 (br, 2H), 7.12 (br, 2H), 6.92 (br, 2H), 6.77 (br, 1H), 4.80 (br, 2H), 2.89 (br, 4H), 2.21 (br, 2H), 1.24–1.39 (br, 76H), 0.86 (br, 15H).
:
1H NMR (500 MHz, CDCl3) δ 8.03 (br, 1H), 7.76 (br, 2H), 7.49 (br, 3H), 7.10 (br, 3H), 6.92 (br, 2H), 6.77 (br, 1H), 2.75–2.90 (br, 6H), 1.26–1.73 (br, 16H), 0.89–1.06 (br, 12H). P4
:
1H NMR (500 MHz, CDCl3, δ) 8.08 (br, 1H), 7.81 (br, 2H), 7.55 (br, 3H), 7.15 (br, 3H), 6.93 (br, 1H), 2.92 (br, 4H), 2.74 (br, 2H), 1.26–1.57 (br, 63H), 0.86 (br, 12H).
Footnote |
| † Electronic supplementary information (ESI) available: Synthesis of intermediates, 1H NMR spectra, and CV traces. See DOI: https://doi.org/10.1039/d2ma00116k |
| This journal is © The Royal Society of Chemistry 2022 |