Abstract
We have used Suzuki coupling to synthesize a series of maleimide–thiophene copolymers presenting pendent 2-hydroxyethyl and 6-hydroxyhexyl units. The maleimide–thiophene copolymers containing different contents of OH groups were then reacted with 3,3′-dimethoxy-4,4′-biphenylene diisocyanate (DMBPI) in solution to form the interchain-linked polymers. The interchain-linked polymers exhibited excellent solubility in organic solvents. The average molecular weight and thermal stability of the copolymers increased after interchain linking with DMBPI. The wavelengths of maximum absorption of the interchain-linked copolymers were red-shifted relative to those of the corresponding side-chain copolymers. The energy level of the lowest unoccupied molecular orbitals and highest occupied molecular orbitals decreased after the copolymers had undergone interchain linking with DMBPI. We fabricated polymer solar cells (PSCs) from blends of the interchain-linked copolymers and [6,6]-phenyl-C61-butyric acid methyl ester. The photovoltaic performances of the PSCs incorporating the interchain-linked copolymers were superior to those of the corresponding PSCs based on the OH-presenting copolymers.
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Introduction
The development of novel low-band gap π-conjugated polymers is an attractive research area because bulk heterojunction polymer solar cells (PSCs) incorporating them can be fabricated at low cost with large areas, flexible shapes, light weight and solution processability.1, 2, 3, 4, 5, 6 The photoactive layer in most bulk heterojunction cells is based on a blend of an electron–donor conjugated polymer and an electron–acceptor fullerene derivative, typically [6,6]-phenyl-C61-butyric acid methyl ester (PCBM). Several recent efforts have focused on the synthesis of a new low-band gap conjugated polymers that improve the absorption of solar radiation and increase charge mobilities.7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20 In addition to the intrinsic characteristics of the polymer, the amount of PCBM in the blend,17, 18 the compatibility of the polymer and PCBM, the morphology of the photoactive layer19, 20, 21 and the device-processing conditions all have important roles affecting the photovoltaic (PV) performance of PSCs.8, 9, 10, 22, 23 Photo-energy conversion efficiencies (η) of >7% have been achieved for PSCs based on blends of poly(thiophene) derivatives and fullerene derivatives.7, 8, 9, 10, 24, 25
In addition to the short-circuit current densities (JSC) and values of η that are typically measured, recent investigations have also been made into optimizing the PV efficiency stability of PSCs. For example, incorporation of a ultraviolet (UV) shielding layer into a PSC can protect the cell from damage caused by UV light and enhance the operational stability.26, 27 Inserting the buffer layer (ZnO, MnO, Cs2CO3 or Al2O3 thin film) at the interface between the electrode and the photoactive layer can not only prevent the O2/H2O-induced degradation of the PSC but also provide a larger electron extraction interface and, therefore, an enhanced photocurrent density.28, 29, 30, 31, 32 In addition, the PV performance is strongly related to the morphology of the active layer based on a conjugated polymer/PCBM blend. Some approaches have been tested to control the nanoscale film morphologies of polymer/PCBM blends.33, 34, 35, 36 The addition of a compatibilizer to suppress large-scale phase separation of the polymer/PCBM blend can enhance the long-term thermal stability of the cell performance.33 Incorporating electron acceptors with high mobility in the polymer/PCBM blend film can result in highly balanced electron and hole mobilities, thereby enhancing the PV performance of the PSC.34 Light- or solvent-soaking to tailor the morphology of the active layer is another potential approach toward improving the PV stabilities of PSCs.35, 36 On the other hand, decreased PV efficiency stability is closely related to the degree of thermally induced aggregation of the polymer chains and PCBM units.37, 38, 39 Thermally crosslinkable fullerene derivatives have been used to improve the thermal stabilities of PSCs by chemically fixing the optimized morphology of the photoactive layer.40, 41, 42, 43, 44 Moreover, photo-crosslinkable polythiophene derivatives have also been developed to stabilize the thin-film morphology of the photoactive layer, thereby enhancing the stability of PSCs.45, 46, 47 In addition, new PSCs fabricated from the thermal-crosslinked polymers have been reported to possess enhanced morphological stability.48, 49
In this study, we synthesized a series of maleimide–thiophene copolymers containing different contents of OH groups, which we then interchain-linked with 3,3′-dimethoxy-4,4′-biphenylene diisocyanate (DMBPI) to form lightly crosslinked copolymers. Here, DMBPI plays the role of a chain extender of the copolymers. The average molecular weights of the copolymers were enhanced after forming the bridge links with DMBPI. We anticipated higher thermal stability and better thin-film formability for the interchain-linked copolymers relative to those of their corresponding OH group-presenting side-chain copolymers.50 The PV performance of the OH group-containing side-chain maleimide–thiophene copolymers has been reported by us previously.50 However, PV properties of the PSCs fabricated from these OH group-containing side-chain maleimide–thiophene copolymers were poor owing to low molecular weight and poor thin-film quality of the copolymers. The improvement of the thin-film formability and the stability of the polythiophene derivatives by the interchain-linking based on the diisocyanate chemistry has not been reported before even though the photo- and thermal-crosslinkable polythiophene derivatives have been developed to enhance the thermal stability of the photoactive layer. We fabricated a series of PSCs from the blends of the copolymers (either OH group-presenting side-chain copolymers or interchain-linked copolymers) with the fullerene derivative PCBM. Maleimide polymers are well-established red emitters in polymer light-emitting devices.51, 52 Moreover, a low-band gap polymer providing high charge mobility is a good choice for use as the electron-donating polymer when preparing PSCs exhibiting efficient photon-to-charge conversion. Therefore, we chose maleimide–thiophene copolymers as electron-donating polymers for our PSCs. We expected the PV performance and operational stability of the PSCs to be enhanced by the presence of the DMBPI bridge links between the backbones of the maleimide–thiophene copolymers. We used UV–visible (Vis) absorption spectroscopy and cyclic voltammetry to study the effects of the DMBPI bridge links on the photophysical and electrochemical behavior, respectively, of the copolymers. We also used atomic force microscopy (AFM) to study the morphologies of the OH-functionalized copolymer/PCBM and interchain-linked maleimide–thiophene copolymer/PCBM blends. Herein, we also discuss the influence of the functionality and the degree of DMBPI bridge linking on the morphologies and PV performances of PSCs based on these maleimide–thiophene copolymer/PCBM blends.
Experimental procedure
Synthesis of maleimide–thiophene copolymers
All reactions and manipulations were performed under a N2 atmosphere using standard Schlenk techniques. Chromatographic separations were performed through silica gel. All chemicals were purchased in reagent grade from Aldrich (St Louis, MO, USA), Fluka (Buchs SG, Switzerland) or RDH Chemical (Seelze, Germany). N-(2′-ethylhexyl)-bis(4-bromophenyl)maleimide (1), N-2-(tetrahydro-2H-pyran-2-yloxy)ethyl-3,4-dibromophenyl maleimide (2) and 2,5-bis(4,4,5,5-tetramethyl-1,3,2-dioxaborolan-2-yl)thiophene (4) were synthesized as described previously.50 Scheme 1 details the syntheses of the maleimide–thiophene copolymers TM2C41-OH–TM6C21-OH containing 2-hydroxyethyl and 6-hydroxyhexyl units. The copolymers TM2C41-P, TM2C21-P, TM2C41-OH and TM2C21-OH were synthesized as described previously.50, 53 All of the polymers were prepared through palladium-catalyzed Suzuki coupling polymerization. As displayed in the Scheme 2, the maleimide–thiophene copolymers containing different contents of OH groups were reacted with DMBPI to form the interchain-linked polymers CTM2C41–CTM6C21.54 The chemical structures of the conjugated polymers were characterized using proton nuclear magnetic resonance (1H-NMR) spectroscopy. The average molecular weights of the polymers were characterized using gel permeation chromatography.
N-6-(tetrahydro-2H-pyran-2-yloxy)hexyl-3, 4-dibromophenyl maleimide (3)
Bis(4-bromophenyl)maleimide (2.80 g, 6.90 mmol) was treated with potassium tert-butoxide (1.54 g, 13.8 mmol) in dimethylformamide (20 ml) at 0 °C. After 2 h of stirring, 2-(6-bromohexyloxy)tetrahydro-2H-pyran (1.81 g, 13.8 mmol) was added to the solution, which was then stirred at room temperature for 10 h. After evaporating the volatiles under reduced pressure, the residue was dissolved in EtOAc and washed with water. The organic phase was dried and concentrated. The desired product was isolated through column chromatography (EtOAc/hexanes) as a yellow liquid (2.8 g, 69%). 1H-NMR (600 MHz, CDCl3): δ 1.30–1.42 (m, 8H), 1.44–1.58 (m, 4H), 1.65–1.80 (m, 2H), 3.72 (t, 2H), 3.81 (t, 2H), 3.94 (t, 2H), 4.54 (t, 1H), 7.34 (d, 4H) and 7.48 (d, 4H) p.p.m. Anal. Calcd. for C27H29NO4Br2: C, 54.6%; H, 4.98%; O, 10.90%; and N, 2.37%. Found: C, 53.9%; H, 4.93%; O, 11.03%; and N, 2.54%.
Copolymer TM6C41-OH
Compounds 1 (0.62 g, 1.2 mmol), 3 (0.17 g, 0.30 mmol), 4 (0.50 g, 1.5 mmol) and Pd(PPh3)4 (0.020 g, 0.017 mmol) were dissolved in a mixture of toluene (10 ml) and aqueous K2CO3 (1.38 g) in H2O (5 ml). The solution was heated under reflux with vigorous stirring for 24 h. Next, the end-capper, 4-bromotoluene (0.58 ml, 3.4 mmol), was added, together with additional Pd(PPh3)4, and then the reaction mixture was heated under reflux for a further 24 h. After cooling to room temperature, the volatiles were evaporated under reduced pressure and the aqueous residue extracted with toluene. The combined extracts were dried (MgSO4), filtered and concentrated to yield the polymer TM6C41-P, which was dissolved in tetrahydrofuran (THF). Thirty-seven percent HCl (5 ml) was added dropwise to the polymer solution, which was then heated under reflux for 12 h. After cooling to room temperature, the volatiles were evaporated under reduced pressure. The residue was dissolved in a small amount of THF and precipitated with MeOH/H2O (10:1 (v v−1)); this procedure was repeated several times. The purified polymer was filtered and dried under vacuum to yield a red solid powder (0.55 g, 48%). Mn=1.92 kg mol−1; Mw=4.28 kg mol−1. 1H-NMR (600 MHz, CDCl3): δ 0.80–0.95 (m, 24H), 1.15–1.45 (m, 32H), 1.46–1.64 (m, 8H), 1.74–1.84 (m, 4H), 3.50–3.56 (d, 8H), 3.61–3.67 (m, 4H), 7.32–7.41 (m, 40H) and 7.47–7.64 (m, 10H) p.p.m. Anal. Calcd. for [(C28H27NO2S)4(C26H23NO3S)]: C, 75.50%; H, 5.98%; O, 8.08%; N, 3.17%; and S, 7.27%. Found: C, 74.9%; H, 5.87%; O, 8.38%; N, 3.27%; and S, 7.20%.
Copolymer TM6C21-OH
The reaction of 1 (0.514 g, 1.0 mmol), 3 (0.290 g, 0.5 mmol), 4 (0.500 g, 1.50 mmol), Pd(PPh3)4 (0.020 g, 0.017 mmol), K2CO3 (1.38 g), H2O (2 ml) and 4-bromotoluene (0.58 ml, 3.4 mmol) was performed using the same procedure as that described above for TM6C41-P to provide a red solid powder (0.42 g, 34%). Mn=2.15 kg mol−1; Mw=3.87 kg mol−1. 1H-NMR (600 MHz, CDCl3): δ 0.80–0.95 (m, 12H), 1.15–1.45 (m, 16H), 1.46–1.64 (m, 8H), 1.74–1.84 (m, 2H), 3.50–3.56 (d, 4H), 3.61–3.67 (m, 4H), 7.32–7.41 (m, 24H) and 7.47–7.64 (m, 6H) p.p.m. Anal. Calcd. for [(C28H27NO2S)2.16(C26H23NO3S)]: C, 75.21%; H, 5.79%; O, 8.48%; N, 3.20%; and S, 7.32%. Found: C, 75.30%; H, 5.62%; O, 8.57%; N, 3.12%; and S, 7.10%.
CTM2C41
TM2C41-OH (0.2 g, 27.4 μmol) and DMBPI (8.1 mg, 27.4 μmol) were dissolved in a mixture of anhydrous THF and dimethylformamide (10:1 (v v−1); 30 ml) under a N2 atmosphere.51 The solution was heated under reflux with vigorous stirring for 6 h. After cooling to room temperature, the volatiles were evaporated under reduced pressure. The residue was dissolved in a small amount of THF and precipitated with MeOH; this procedure was repeated several times. The purified polymer was filtered and dried under vacuum to yield a red solid powder (0.16 g). Mn=5.29 kg mol−1; Mw=8.41 kg mol−1. 1H-NMR (600 MHz, CDCl3): δ 0.80–1.0 (m, 24H), 1.20–1.40 (m, 35H), 1.75–1.83 (m, 4H), 3.55 (d, 8H), 3.85–3.92 (m, 4H), 7.1 (d, 2H), 7.2–7.5 (m, 10H) and 7.5–7.7 (m, 20H) p.p.m.
CTM2C21
The reaction of TM2C21-OH (0.2 g, 33 μmol) and DMBPI (9.8 mg, 33 μmol) was performed using the same procedure as that described above for CTM2C41. The purified polymer was filtered and dried under vacuum to yield a red solid powder (0.17 g). Mn=5.94 kg mol−1; Mw=8.26 kg mol−1. 1H-NMR (600 MHz, CDCl3): δ 0.80–1.0 (m, 15H), 1.20–1.40 (m, 23H), 1.75–1.83 (m, 2.5H), 3.58 (d, 5H), 3.80–3.92 (m, 3H), 7.05 (d, 2H), 7.2–7.5 (m, 10H) and 7.5–7.7 (m, 20H) p.p.m.
CTM6C41
The reaction of TM6C41-OH (0.2 g, 46.7 μmol) and DMBPI (14 mg, 46.7 μmol) was performed using the same procedure as that described above for CTM2C41. The purified polymer was filtered and dried under vacuum to yield a red solid powder (0.15 g). Mn=2.92 kg mol−1; Mw=4.64 kg mol−1. 1H-NMR (600 MHz, CDCl3): δ 0.80–0.95 (m, 24H), 1.15–1.45 (m, 32H), 1.46–1.64 (m, 8H), 1.74–1.84 (m, 4H), 3.50–3.56 (d, 8H), 3.61–4.00 (m, 4H), 6.95–7.2 (m, nH), 7.32–7.41 (m, 10H) and 7.47–7.64 (m, 40H) p.p.m.
CTM6C21
The reaction of TM6C21-OH (0.2 g, 35 μmol) and DMBPI (10 mg, 35 μmol) was performed using the same procedure as that described above for CTM2C21. The purified polymer was filtered and dried under vacuum to yield a red solid powder (0.18 g). Mn=3.85 kg mol−1; Mw=5.70 kg mol−1. 1H-NMR (600 MHz, CDCl3): δ 0.80–0.95 (m, 12H), 1.15–1.45 (m, 16H), 1.46–1.64 (m, 8H), 1.74–1.84 (m, 2H), 3.50–3.56 (d, 4H), 3.61–4.00 (m, 4H), 6.95–7.20 (m, nH), 7.32–7.41 (m, 6H) and 7.47–7.64 (m, 24H) p.p.m.
Instruments
1H-NMR spectra were recorded using a Bruker AMX-600 MHz spectrometer (Bruker Co., Billerica, MA, USA). Elemental analysis was performed using an elemental analyzer (Elementar Vario EL III; Hanau, Germany). Gel permeation chromatography was performed using a Waters chromatography system (Waters 717 Plus Autosampler, Waters Co., Milford, MA, USA), two Waters Styragel linear columns, polystyrene as the standard and THF as the eluent. Glass transition temperatures (Tg) were measured under a N2 atmosphere using a differential scanning calorimeter (DSC-2010; TA Instruments, New Castle, DE, USA) operated at a heating rate of 10 °C min−1. Thermogravimetric analysis was performed under a N2 atmosphere using a thermogravimetric analyzer (TGA-2050; TA Instruments) operated at a heating rate of 10 °C min−1. UV–Vis spectra were recorded using a Hewlett-Packard 8453 spectrophotometer (Hewlett-Packard Taiwan Co., Taipei, Taiwan). Photoluminescence spectra were recorded using a Hitachi F-4500 fluorescence spectrophotometer (Hitachi High-Tech Co., Tokyo, Japan). The redox potentials of the polymers were determined through cyclic voltammetry, using a BAS 100B electrochemical analyzer (Bioanalytical Co., West Lafayette, IN, USA) operated at a scanning rate of 100 mV s−1; the polymer was dissolved in deoxygenated dry dimethylformamide containing 0.1 M tetra-n-butylammonium hexafluorophosphate as the electrolyte; the working electrode was Pt and the reference electrode was saturated non-aqueous Ag/AgCl; ferrocene was used for potential calibration (all reported potentials are referenced against Ag/Ag+); and for determining reversibility criteria. The morphologies of the polymer solid films were observed using a Digital Instruments Dimension 3100 Series scanning probe microscope (Veeco Instruments, Plainview, NY, USA).
PSC device fabrication and characterization
The PSCs had the following structure: indium tin oxide-coated glass/hole-transporting material/polymer:PCBM (90–100 nm)/LiF (0.5 nm)/Al (100 nm). The indium tin oxide-coated glass, having a sheet resistance of 20 Ω sq−1, was purchased from Applied Film Corporation (AF Co., Alzenau, Germany). The PSC fabrication was based on an interpenetrating network of the conjugated polymer and the fullerene derivative PCBM, which was purchased from American Dye Source (ADS Co., Baie Durfe, Quebec, Canada) and used as received. Solutions (30 mg ml−1) of the conjugated polymer and PCBM were prepared at different weight ratios in cyclohexanone (CHO). The PSCs were prepared as follows: glass substrates with patterned indium tin oxide electrodes were washed well and then cleaned through O2 plasma treatment. A thin film of the hole-transporting material—poly(3,4-ethylenedioxythiophene) doped with polystyrenesulfonate (PEDOT:PSS, AI4083; Heraeus Clevios Co., Hanau, Germany)—was deposited on the indium tin oxide layer of the glass substrate using a spin-casting method. The conjugated polymer/PCBM composite film was spin-coated (1500 r.p.m.) from the CHO solution (30 mg ml−1) onto the hole-transporting material layer and then dried at 80 °C for 1 h in a glove box. The LiF/Al-based cathode was thermally deposited, in a high-vacuum chamber, onto the photoactive thin film based on the conjugated polymer/PCBM blend. The active area of the PSC was 0.04 cm2. After electrode deposition, the PSC was encapsulated. The cathode deposition rate was determined using a quartz thickness monitor (STM-100/MF; Sycon Instruments, East Syracuse, NY, USA). The thickness of the thin film was determined using a surface texture analysis system (3030ST; Dektak, Veeco Instruments). The PV properties of the PSCs were measured using a programmable electrometer with current and voltage sources (Keithley 2400; Keithley Instruments, Inc., Cleveland, OH, USA) under the illumination of solar light (100 mW cm−2) from an AM1.5 solar simulator (NewPort Oriel 96000; Newport Corporation Taiwan, Taipei, Taiwan).
Results and Discussion
Characterization of the chemical structure and thermal properties of the interchain-linked copolymers
Figure 1a presents the 1H-NMR spectrum of the 6-hydroxyhexyl-functionalized maleimide–thiophene copolymer TM6C21-OH. The signals for protons g and (h+i) appear at δ 3.5–3.6 and 3.6–3.7 p.p.m., respectively, with relative integrals of 5.19 and 4.81, respectively, suggesting that the molar percentage of the 6-hydroxyhexyl-functionalized maleimide–thiophene units was 31.6 mol%. Accordingly, the molar percentage of 6-hydroxyhexyl-functionalized maleimide–thiophene units in TM6C41-OH was 19.7 mol%. In addition, the molar percentages of the 2-hydroxyethyl-functionalized maleimide–thiophene units in TM2C41-OH and TM2C21-OH were 18.9% and 28.6%, respectively.50 The chemical shifts and relative intensities of the signals were in agreement with the proposed structures for these conjugated polymers. Figure 1b displays the 1H-NMR spectrum of the interchain-linked maleimide–thiophene copolymer CTM6C21. Relative to the corresponding signal for TM6C21-OH, the signal of proton i shifted to lower field after the OH groups had been reacted with DMBPI, appearing at δ 3.88–4.00 p.p.m. (proton i′). The signal of protons (i′+r′) appeared at δ 3.88–4.00 p.p.m. for CTM6C21 with a relative integral of 2.43. Notably, the bridge linking of the OH groups was incomplete: a signal for protons i of the interchain-linked copolymer CTM6C21 remained at δ 3.6–3.7 p.p.m., albeit with diminished absorption intensity. The relative absorption intensity of proton i′ indicates that 36.0 mol% of the OH groups had reacted with DMBPI. In addition, the 1H-NMR spectrum of CTM6C41 indicated that 41.5 mol% of the OH groups had reacted with DMBPI. To prevent gelation of the copolymer, the degree of bridge-linked OH groups was controlled through the addition of an appropriate amount of DMBPI during the reaction procedure. The lightly interchain-linked copolymers exhibited good solubilities in organic solvents. The 1H-NMR spectrum of the interchain-linked maleimide–thiophene copolymer CTM2C21 featured signals for protons (h+i) and (i′+r′) in the range δ 3.8–4.0 p.p.m. (Figure 2). The signals for protons (i′+r′) were overlapped with that of the protons (h+i). Therefore, we could not calculate the degree of bridge linking through DMBPI for CTM2C21. We observed the same behavior for CTM2C41. Nevertheless, we could confirm that interchain linking through DMBPI had occurred for CTM2C41 and CTM2C21.
The number- and weight-average molecular weights of the 2-hydroxyethyl- and 6-hydroxyhexyl-presenting maleimide–thiophene copolymers TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH were ca. 1.92–5.94 and 3.87–8.41 kg mol−1, respectively (Table 1). Moreover, gel permeation chromatography analysis indicated that the number- and weight-average molecular weights of the interchain-linked copolymers were greater than those of the 2-hydroxyethyl- and 6-hydroxyhexyl-presenting copolymers, suggesting that the OH-containing side-chain copolymers had reacted with DMBPI to form interchain-linked polymers. We attribute the higher average molecular weights for the interchain-linked copolymers to the thermal reaction of DMBPI with the OH-containing side-chain copolymers.
The operational stability of a PSC device is directly related to the thermal stability of its conjugated polymers. Thus, high glass transition (Tg) and thermal degradation (Td) temperatures are desirable if a conjugated polymer is to be applied in PSCs. Supplementary Figure S1 displays DSC thermograms of the OH-containing side-chain copolymers and interchain-linked copolymers. The values of Tg of the OH-presenting copolymers TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH were 86, 90, 53 and 56 °C, respectively (Table 1); notably, the values of Tg for the 2-hydroxyethyl-presenting copolymers (TM2C41-OH, TM2C21-OH) were higher than those of the 6-hydroxyhexyl-presenting copolymers (TM6C41-OH, TM6C21-OH), presumably because of the lengths of their ethyl and hexyl side chains. Moreover, the values of Tg of the interchain-linked copolymers CTM2C41, CM2C21, CTM6C41 and CTM6C21 were 105, 113, 94 and 66 °C, respectively. Thus, the interchain-linked copolymers possessed higher values of Tg than did the corresponding OH-presenting copolymers, presumably because of greater average molecular weights and decreased polymer chain mobility. After interchain linking through DMBPI, the enhancement in the values of Tg was more pronounced for the copolymers CTM6C41 and CTM6C21 than for the copolymers CTM2C41 and CM2C21, possibly because of the greater degree of bridge linking of the former pair. The 5% weight loss temperatures (Td) of the OH-presenting copolymers TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH were 303, 287, 298 and 237 °C, respectively (Table 1). Thus, the value of Td decreased upon increasing the content of side-chain units, presumably because of the presence of OH-containing alkyl side chains. Moreover, the 2-hydroxyethyl-presenting copolymers provided higher values of Td than did the 6-hydroxyhexyl-presenting copolymers, presumably because their shorter alkyl side chains led to the greater thermal stability. In addition, the values of Td of the interchain-linked copolymers CTM2C41, CM2C21, CTM6C41 and CTM6C21 were 313, 350, 305 and 334 °C, respectively; these values are higher than those of the corresponding side-chain copolymers because of the effect of bridge linking through the DMBPI units.
The copolymers TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH had good solubilities in most organic solvents, including CHO, xylene, toluene, THF, CH2Cl2, CHCl3 and chlorobenzene (Table 2). In contrast, the interchain-linked copolymers CTM2C41, CTM2C21, CTM6C41 and CTM6C21 had low solubilities in most organic solvents, with the exception of CHO. This behavior is consistent with polar copolymers being more soluble in more polar solvents (for example, CHO).
Optical properties of the maleimide–thiophene copolymers
Figure 3 presents normalized UV–Vis absorption spectra of the OH-containing side-chain copolymers and interchain-linked copolymers in CHO solution (concentration: 1 mg ml−1) and as solid films (thickness: 90–100 nm). In Figure 3a, the 2-hydroxyethyl- and 6-hydroxyhexyl-functionalized copolymers (TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH) in CHO solution exhibited their maximum absorption bands centered at approximately 448 nm, with a corresponding additional absorption peak at 325 nm. We attribute the major absorption peak to the π–π* electronic transition of the conjugated polymer backbone. Slight red-shifting of the absorption peaks occurred for the 2-hydroxyethyl-functionalized copolymers TM2C41-OH and TM2C21-OH relative to those of 6-hydroxyhexyl-functionalized copolymers TM6C41-OH and TM6C21-OH. We suspect that the presence of the longer alkyl side chains led to greater degrees of twisting of the polymer backbone, thereby shortening the effective conjugation lengths in the copolymers TM6C41-OH and TM6C21-OH relative to those in the copolymers TM2C41-OH and TM2C21-OH. In addition, we observed red-shifts and enhanced full-widths at half-maximum of the absorption peaks for the copolymers in the form of solid films, relative to those in solution, presumably because of interactions between and aggregation of the polymer chains in the solid film. Moreover, in the form of solid films, slight red-shifting of the absorption peaks occurred for the 2-hydroxyethyl-functionalized copolymers relative to those of 6-hydroxyhexyl-functionalized copolymers. In addition, Figure 3b presents normalized UV–Vis absorption spectra of the interchain-linked copolymers in CHO solution and as solid films. Notably, only slight differences existed in the absorption behavior of the interchain-linked copolymers relative to that of the corresponding OH-containing side-chain copolymers. We attribute the enhanced intensity of the absorption peak at 325 nm for the interchain-linked copolymers, relative to that of the side-chain copolymers, to the absorption of the DMBPI-derived linker between the polymer backbones. In CHO, DMBPI exhibits its maximum absorption wavelength at 300 nm.
Electrochemical properties of the maleimide–thiophene copolymers
We employed cyclic voltammetry to investigate the electrochemical behavior of the conjugated polymers and to estimate the energy levels of their highest occupied molecular orbitals (HOMOs) and lowest unoccupied molecular orbitals (LUMOs). We calculated the HOMO energy levels of the copolymers from their onset potentials for oxidation by assuming that the absolute energy level of Ag/Ag+ was −4.71 V below the vacuum level; we calculated LUMO energy levels from the HOMO energy levels and the absorption edge.53 Figure 4 displays cyclic voltammetry traces of the OH-containing side-chain copolymers and interchain-linked copolymers; Table 3 summarizes the electrochemical properties of the copolymers. The cyclic voltammograms of TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH revealed oxidation onset potentials (Eoxonset) at 0.80, 0.85, 0.83 and 0.87 V, respectively; that is, the value of Eoxonset increased upon increasing the content of OH groups in the copolymers, presumably because they induced an increased degree of twisting of the polymer backbone, out of planarity.55 Such twisting of the polymer backbone decreased the effective conjugation length, thereby enhancing the value of Eoxonset.55 In addition, the values of Eoxonset for the 6-hydroxyhexyl-functionalized copolymers were higher than those of the 2-hydroxyethyl-functionalized copolymers. This observation implies that the presence of 6-hydroxyhexyl groups twisted the polymer backbone more significantly than did the presence of 2-hydroxyethyl groups. The LUMO energy levels of TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH were −3.21, −3.25, −3.22 and −3.25 eV, respectively; the HOMO energy levels were −5.51, −5.56, −5.54 and −5.58 eV, respectively. Thus, for the OH-containing side-chain copolymers, the LUMO and HOMO energy levels decreased upon increasing the content of OH groups. The decrease in the HOMO energy level upon increasing the OH group content corresponds with the increased value of Eoxonset.55 Moreover, the HOMO energy levels of the 6-hydroxyhexyl-functionalized copolymers were lower than those of the 2-hydroxyethyl-functionalized copolymers. On the other hand, the optical band gap of each copolymer, determined from the absorption edge, was approximately 2.3 eV. Thus, the optical band gap did not vary significantly with respect to the OH group content. As a result, the LUMO energy levels for the copolymers decreased upon increasing the OH group content.
Furthermore, the values of Eoxonset for the interchain-linked copolymers were higher than those of the corresponding OH-containing side-chain copolymers. The LUMO energy levels for CTM2C41, CTM2C21, CTM6C41 and CTM6C21 were −3.25, −3.26, −3.25 and −3.28 eV, respectively; their HOMO energy levels were −5.55, −5.57, −5.57 and −5.61 eV, respectively. Relative to those of the OH-presenting copolymers, the values of Eoxonset were further enhanced after bridging the side chains of the copolymers through DMBPI units. Such interchain linking increased the degree of twisting of the polymer backbone, thereby decreasing the effective conjugation length and, accordingly, increasing the value of Eoxonset.55 We observed higher values of Eoxonset for CTM6C41 and CTM6C21 relative to those of TM6C41-OH and TM6C21-OH, presumably because of the higher degree of bridging through DMBPI units for CTM6C41 and CTM6C21. In addition, the decrease in the HOMO energy level upon increasing the degree of bridge linking correlated with the increase in the value of Eoxonset.55 Because the optical band gap did not vary significantly with respect to the degree of bridge linking of the copolymers, the interchain-linked copolymers possessed lower LUMO energy levels relative to those of the corresponding OH-containing side-chain copolymers.
Optical properties and morphologies of maleimide–thiophene copolymer/PCBM blend films
Supplementary Figure S2 presents normalized UV–Vis absorption spectra of OH-containing side-chain copolymer/PCBM and interchain-linked copolymer/PCBM blend films prepared at various weight ratios. The absorption bands of the conjugated copolymers extended from 360 to 700 nm, whereas that of PCBM ranged from 300 to 360 nm. The maximum absorptions of the conjugated copolymers and PCBM appeared at approximately 450 and 325 nm, respectively. Moreover, for the maleimide–thiophene copolymer/PCBM blend films, the absorption intensity of the conjugated copolymer decreased upon increasing the PCBM content. Notably, the absorption behaviors of the OH-containing side-chain copolymer/PCBM and interchain-linked copolymer/PCBM blend films were similar.
We used AFM to investigate the compatibility and morphology of the maleimide–thiophene copolymer/PCBM blend films, because the PV properties of PSCs are closely related to the morphology within the photoactive polymer blend. Supplementary Figure S3 displays topographic and phase images of the TM2C41-OH/PCBM (1:4 (w/w)) and TM2C21-OH/PCBM (1:4 (w/w)) blend films, respectively, after they had been annealed at 80 °C for 1 h.50 Table 4 summarizes the roughnesses of the composite films. For the TM2C41-OH/PCBM blend films, the presence of the hydrogen bonds between the OH groups of TM2C41-OH and the ester group of PCBM enhanced the compatibility of the components. As a result, the PCBM units were mixed uniformly in the TM2C41-OH/PCBM blend films. In Supplementary Figure S3, we do not observe a phase-separated interpenetrating network with sizable PCBM domains for the TM2C41-OH/PCBM blend film incorporating a high PCBM content (1:4 (w/w)). In contrast, we observed a phase-separated interpenetrating network with PCBM domains for the TM2C21-OH/PCBM composite film featuring a low PCBM content (1:1 (w/w)), presumably because the high content of OH groups of TM2C21-OH led to significant hydrogen bonding among the OH groups and, therefore, self-aggregation of the conjugated polymer chains. Self-aggregation of the polymer chains led to the high contrast ratios for the PCBM domains and TM2C21-OH matrix in the phase images of the TM2C21-OH/PCBM blend films. In addition, the surface morphologies of the TM2C41-OH/PCBM composite films did not vary significantly upon increasing the PCBM content. Although we observed greater surface roughnesses for blend films incorporating the copolymer featuring the higher OH group content, the distribution of PCBM domains in the TM2C21-OH/PCBM blend films was suitable for electron transport in PSCs. Figure 5 displays topographic and phase images of the TM6C41-OH/PCBM and TM6C21-OH/PCBM blend films, respectively, after they had been annealed at 80 °C for 1 h. These AFM images indicate that the PCBM units were mixed uniformly in the TM6C41-OH/PCBM blend films, due to the presence of hydrogen bonds among the OH groups of TM6C41-OH and the ester group of PCBM. Moreover, we also observed good compatibility for the TM6C21-OH/PCBM blend film (1:4 (w/w)). Self-aggregation of the polymer chains, as a result of the high OH group content of TM6C21-OH, did not occur in the blend films of TM6C21-OH/PCBM, presumably because of dilution of the long side-chain groups. We did not observe a high contrast ratio for the PCBM domains and polymer matrix in the phase image of the TM6C21-OH/PCBM blend film.
Figures 6 and 7 present phase images of the interchain-linked copolymer (CTM2C41, CTM2C21, CTM6C41 and CTM6C21)/PCBM blend films. Although the morphologies of the CTM2C41/PCBM (1:1 and 1:4, w/w) blend films were quite distinct from those of the TM2C41-OH/PCBM blend films, the phase images revealed the uniform distribution of PCBM units in the CTM2C41 matrix, due to the lower content of OH groups and the lower degree of the interchain linking through DMBPI units. In addition, for the CTM2C21/PCBM composite films we observed phase-separated interpenetrating networks with PCBM domains. The size of the PCBM domains in CTM2C21 was much smaller than that in TM2C21-OH, presumably because the content of OH groups was lower after forming the bridging links through DMBPI units. As a result, self-aggregation of the conjugated polymer chains was prevented in the blend film. The PCBM and conjugated polymer units in CTM2C21/PCBM blend films had greater compatibility than that in the TM2C21-OH/PCBM blend films. Nevertheless, the phase images of the interchain-linked copolymer (CTM6C41, CTM6C21)/PCBM blend films were similar to those of the CTM2C41/PCBM blend films. The phase images revealed the uniform distributions of PCBM units in the CTM6C41 and CTM6C21 matrices, except in the CTM6C21/PCBM (1:4 (w/w)) blend film, presumably because the higher degree of bridging links through DMBPI units decreased the compatibility between the polymer chains and the PCBM units in the CTM6C21/PCBM blend film.
PV properties of PSCs based on maleimide–thiophene copolymer/PCBM blend films
We fabricated PSCs incorporating films of maleimide–thiophene copolymer/PCBM blends prepared from CHO solutions using an optimized spin-coating procedure. The photoactive layers based on copolymer (TM2C41-OH, TM2C21-OH, TM6C41-OH and TM6C21-OH)/PCBM blends were thermally treated at 80 °C for 1 h. Figure 8 displays the photocurrent density–voltage plots of the PSCs we fabricated from maleimide–thiophene copolymer/PCBM blend films of various weight ratios. Table 4 summarizes the PV properties of these PSCs, including their open-circuit voltages (VOC), short-circuit current densities (JSC), fill factors and photo-energy conversion efficiencies (η). For the OH-containing side-chain copolymer/PCBM-based PSCs (PSC AI-1–PSC AIV-3), the values of JSC and η increased upon increasing the PCBM content, whereas the values of VOC followed the opposite trend. Higher concentrations of PCBM favored the formation of phase-separated interpenetrating networks with sizable domains in the photoactive layer,56, 57 in turn favoring effective charge separation;58, 59 as a result, we observed higher values of JSC and η. Conversely, the values of VOC decreased slightly upon increasing the PCBM content. Although the value of VOC is determined mainly by the difference between the LUMO energy level of the electron acceptor (in this case, PCBM) and the HOMO energy level of the electron–donor (the conjugated polymer), it is also affected by the PCBM content because charge transfer occurs between the polymer and PCBM. Consequently, the values of VOC decreased upon increasing the PCBM content.60 In addition, the values of JSC and η for the TM2C21-OH/PCBM-based PSCs (PSC AII-1–PSC AII-3) were higher than those of the TM2C41-OH/PCBM-based PSCs (PSC AI-1–PSC AI-3), presumably because of the presence of more-suitable charge transfer channels in the TM2C21-OH/PCBM blend films. Nevertheless, the values of VOC of the TM2C21-OH/PCBM-based PSCs were not higher than those of the TM2C41-OH/PCBM-based PSCs, even through the HOMO energy level of TM2C21-OH was lower than that of TM2C41-OH. Nevertheless, the influence of the content of OH groups on the PV properties of the PSCs based on the TM6C41-OH/PCBM and TM6C21-OH/PCBM blends (PSC AIII-1–PSC AIII-3 and PSC AIV-1–PSC AIV-3) was the same as those of the PSCs based on TM2C21-OH/PCBM and TM2C41-OH/PCBM. The values of VOC of the 6-hydroxyhexyl-presenting copolymer (TM6C41-OH and TM6C21-OH)/PCBM-based PSCs were slightly higher than those of the 2-hydroxyethyl-presenting copolymer (TM2C41-OH and TM2C21-OH)/PCBM-based PSCs, presumably because the HOMO energy levels of TM6C41-OH and TM6C21-OH were lower than those of TM2C41-OH and TM2C21-OH, respectively. Conversely, the values of JSC and η of the PSCs based on TM6C41-OH/PCBM and TM6C21-OH/PCBM were lower than those of the PSCs based on TM2C41-OH/PCBM and TM2C21-OH/PCBM, presumably because of the differences in the lengths of the alkyl side chains of the copolymers. Longer alkyl side chains led to lower concentrations of the conjugated polymer backbones in the polymer matrices. As a result, we observed a lower hole-transporting capacity for the photoactive layer based on the 6-hydroxyhexyl-presenting copolymer/PCBM blend.
Figure 9 displays the photocurrent density–voltage plots of the PSCs (PSC BI-1–PSC BIV-3) that we fabricated from interchain-linked maleimide–thiophene copolymer (CTM2C41, CTM2C21, CTM6C41 and CTM6C21)/PCBM blend films of various weight ratios); Table 5 summarizes the PV properties of these PSCs. The PV performances of the PSCs based on the interchain-linked copolymers (PSC BI-1–PSC BIV-3) were superior to those of the PSCs based on the 2-hydroxyethyl- and 6-hydroxyhexyl-functionalized copolymers (PSC AI-1–PSC AIV-3). One possible reason for this behavior is that the content of OH groups was lower in the interchain-linked copolymers. The OH groups on the surface of the photoactive layer would have reacted with the Al to form metal oxides, which would resist electron injection from the photoactive layer to the cathode, thereby resulting in low photocurrent densities for these PSC.61 Moreover, the interchain-linked copolymers with higher average molecular weights formed higher-quality thin films than did the corresponding OH-presenting maleimide–thiophene copolymers. A poor-quality polymer film results in a low charge transporting capacity in the photoactive layer. In addition, conjugated polymers with high hole mobilities can be obtained from interchain-linked conjugated polymers featuring a suitable content of conjugated bridges.62 Accordingly, we observed higher values of JSC for the interchain-linked copolymer/PCBM-based PSCs, even though the films of the interchain-linked copolymer/PCBM blends (CTM6C21/PCBM blends) possessed poorer phase-separated morphologies than did those of the corresponding OH-functionalized copolymer/PCBM blends. In addition, we attribute the higher values of VOC of the PSCs based on the interchain-linked copolymer (CTM2C41, CTM2C21, CTM6C41 and CTM6C21)/PCBM blends to the lower HOMO energy levels of the interchain-linked copolymers. Notably, however, the low HOMO energy levels of the interchain-linked copolymers would inhibit hole injection from the photoactive layer to the hole-transporting material layer. Therefore, we observed higher series resistivities and lower fill factors for the PSCs incorporating the interchain-linked copolymer/PCBM blends than those for the PSCs based on the corresponding OH-functionalized copolymer/PCBM blends. Nevertheless, the values of η of the PSCs based on the interchain-linked copolymers were higher than those of the PSCs based on the OH-functionalized copolymers. On the other hand, the PV performances of our PSCs based on the maleimide–thiophene copolymers were lower than those of PSCs based on poly(3-hexylthiophene), presumably because of the low average molecular weight and narrow absorption band of the maleimide–thiophene copolymers. The low average molecular weight resulted in poor-quality polymer films, and thereby, the low charge transporting capacity in the photoactive layer. Nevertheless, the average molecular weights of the maleimide–thiophene copolymers were enhanced through interchain linking of their side-chain groups, thereby enhancing the PV performance of the PSCs based on the maleimide–thiophene copolymers.
In addition to influencing the values of JSC and η, the degree of interchain linking of the maleimide–thiophene copolymer also improved the stability of the PV efficiency. Figure 10 reveals the stabilities of the PV efficiencies of the PSCs based on the maleimide–thiophene copolymer/PCBM (1:4 (w/w)) blend films. We measured the PV efficiencies of these PSCs under illumination (100 mW cm−2) of simulated sunlight from an AM1.5 solar simulator at room temperature. The operational stabilities of the PSCs based on the interchain-linked copolymer/PCBM blends were higher than those of the PSCs based on 2-hydroxyethyl-functionalized copolymer/PCBM blends, as a result of the values of Tg of the interchain-linked copolymers being higher than those of the corresponding OH-containing side-chain copolymers. Moreover, the presence of OH groups in the photoactive layers of the PSCs led to oxidation of the photoactive layers when the conjugated polymers were charged under an electric field, resulting in lower stability for the PSCs fabricated from the OH-presenting side-chain copolymers.61 In addition, during operation of the device, we observed deterioration of the PV performance as a result of the morphological changes of the polymer/PCBM-based photoactive layer. The polymer and PCBM units tended to segregate, with large aggregates of PCBM forming in the film; the PV performance decreased as a result of this phase separation. Therefore, the PSCs fabricated from the interchain-linked polymers having higher values of Tg possessed higher operational stabilities.
Conclusions
We have developed a series of side-chain-type maleimide–thiophene copolymers, presenting different contents of pendent 2-hydroxyethyl and 6-hydroxyhexyl units, for PSC applications. We obtained interchain bridge-linked copolymers through the reactions of the OH groups of the side-chain copolymers with DMBPI. The thermal stabilities of the interchain-linked copolymers were greater than those of the corresponding side-chain copolymers. In addition, the interchain-linked polymers exhibited excellent solubility in CHO. We fabricated a series of PSCs incorporating blends of the fullerene derivative PCBM and either the OH-functionalized or interchain-linked copolymers. The morphology of the photoactive layer and the PV properties of the PSCs were strongly affected by the nature of the pendent functionality and the degree of interchain bridge linking of the conjugated polymers. The PV performances of the PSCs based on the interchain-linked copolymer/PCBM blends were superior to those based on the OH-functionalized copolymer/PCBM blends.
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We thank the National Science Council of Taiwan, ROC, for financial support.
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Lee, RH., Chen, WY. & Shiau, SY. Synthesis and photovoltaic properties of a series of bulk heterojunction solar cells based on interchain-linked conjugated polymers. Polym J 45, 744–757 (2013). https://doi.org/10.1038/pj.2012.212
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DOI: https://doi.org/10.1038/pj.2012.212