Louis-Philippe
Boivin
a,
Mia
Prud’homme
a,
Audrey
Poitras
a,
William
Dupont
a,
Mario
Leclerc
*a and
David
Gendron
*b
aDépartement de Chimie, Université Laval, Québec City, Québec G1V 0A6, Canada. E-mail: mario.leclerc@chm.ulaval.ca
bCégep de Thetford, Kemitek, Thetford Mines Québec, G6G 0A5, Canada. E-mail: dgendron@kemitek.org
First published on 15th July 2025
The growing demand for sustainable materials has spurred interest in biosourced feedstocks and metal-free polymerization techniques for organic electronics. This study explores the synthesis of conjugated polymers using renewable succinic acid-derived monomers through environmentally benign polymerization methods. New pathways were developed to produce three biosourced polymers: poly(phenylene vinylene) (bPPV), poly(cyano-PPV) (bCN-PPV), and poly(thiazolo[5,4-d]thiazole) (bPPTzTz) using Gilch polymerization, Knoevenagel condensation, and Ketcham polymerization, respectively. Comprehensive characterization of these polymers, including molecular weight, optical, electrochemical, and thermal properties, demonstrates their potential for organic electronics. The polymers exhibit high renewable atom content, with polymer bPPV achieving 100% of its atoms coming from succinic acid. This work highlights the feasibility of integrating biosourced monomers and sustainable polymerization strategies, advancing the development of environmentally responsible materials for organic electronics.
One promising alternative to fossil fuels is forest biomass, which consists of carbohydrates (such as cellulose and hemicellulose) and aromatics (such as lignin and tannins).5 Both of these components can be processed into added value compounds.6 Research into cellulosic-derived starting materials has primarily focused on furan-substituted DPP,7 synthesized from succinic acid and furfural. Using lignin derived starting materials, significant progress has been made using vanillin for the synthesis of conjugated polymers. For instance, our group has previously reported the synthesis of heterocycle-substituted benzenes rings using vanillin as a precursor.8 In a subsequent study, we demonstrated their potential by polymerizing them through DArP with diketopyrrolopyrrole (DPP) for transistor applications.9 Additionally, the groups of Kayser10 and Brochon11 have also explored vanillin-based monomers for synthesizing partially bio-sourced conjugated polymers, employing metal-free polymerization methods in both cases.
Since the last decade, only a few metal-free polymerization protocols have been reported.12 Most of these methods rely on the same principle: the condensation of various nucleophiles with carbonyl groups to form alkene derivatives, examples include the aldol condensation,13 the Knoevenagel condensation,14,15 the Horner–Wadsworth–Emmons reaction,16 and polyazomethine synthesis.17 However, other methods utilize a range of organic reactions to achieve conjugated polymers, such as Gilch polymerization,18 the Ketcham reaction,19 Yao et al.'s pyrazine construction,20 and the multicomponent polymerization developed by Kayser et al.10
This study seeks to explore the adaptation of metal-free polymerization techniques to biosourced monomers derived from succinic acid, a renewable feedstock readily obtainable from cellulose.21 By employing dimethyl succinate, we developed novel pathways to conjugated polymers with distinct properties and high renewable atom content. Our approach resulted in the synthesis of three biosourced polymers: poly(phenylene vinylene) (bPPV), cyano-PPV (bCN-PPV), and poly(thiazolo[5,4-d]thiazole) (bPPTzTz), via Gilch polymerization, Knoevenagel condensation, and Ketcham polymerization, respectively.
This paper presents the synthetic methodologies, detailed characterization, and renewable atom content analyses for these polymers. By evaluating their structural, optical, electrochemical, and thermal properties, we aim to highlight the potential of those biosourced materials in reducing reliance on petroleum-based precursors while demonstrating interesting properties required for applications in organic electronics. Through this work, we demonstrate the feasibility of integrating renewable feedstocks into advanced materials development, paving the way for more sustainable approaches to the synthesis of conjugated polymers.
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Scheme 1 Synthesis of PPVs by Gilch polymerization, Knoevenagel condensation and Horner–Wadsorth–Emmons reaction (HWE). |
We oriented our search towards suitable starting materials that can be obtained from biomass. A publication from Short et al. describes that succinic esters could be dimerized and further aromatized into dimethyl 2,5-dihydroxyterephthalate, which features two ester groups.24 These ester groups could then be converted into a variety of functional groups (halomethyl groups, aldehydes groups, nitrile groups, etc.) suitable for different metal-free polymerization protocols. However, we decided to avoid the Horner–Wadsworth–Emmons reaction as it required more synthetic steps to reach the targeted compound than the Gilch and Knoevenagel condensation.
The detailed synthetic procedures can be seen in the ESI,† as well as the 1H and 13C NMR spectra of new intermediate compounds in Fig. S16–S32 (ESI†).
TzTz units have shown great potential in organic electronic. Indeed, they are more electron deficient than their thiophene counterpart which improve the oxidation stability, and they also show strong π–π interaction at the solid state which generally improve charge carrier mobility.34,35 As illustrated in Scheme 4, according to the protocol of Lolaeva et al., the dialdehyde was polymerized into polymer bPPTzTz using dithiooxamide in DMF under microwave heating.19 Initially, we used ethylhexyl side chains, but due to the poor solubility of the resulting material, we opted to increase their length to decyltetradecyl side chains. To achieve this, we modified the previously used procedure for synthesizing compound 7 to incorporate the longer side chains, successfully obtaining monomer 8 with a 75% yield over the three steps from compound 2. Dialdehyde 8 was then polymerized using the Ketcham polymerization method. The resulting polymer was precipitated in methanol and purified via Soxhlet extraction using methanol, acetone, and hexanes. The polymer dissolved in the hexanes fraction and after evaporation of the solvent, polymer bPPTzTz was obtained with a 90% yield.
In our case, the side chains were also biosourced. Both 2-ethylhexyl bromide and 11-(bromomethyl)tricosane were synthesized from their respective alcohols.36 These alcohols, in turn, are produced via the Guerbet reaction using linear alcohols, which are commonly biosourced either from oils and fats (e.g., palm oil, coconut oil)37–39 or by fermentation.40
As shown in Table 1, polymer bPPV consists entirely of atoms (100%) derived from a renewable source (succinic acid). For polymer bCN-PPV, slightly lower but still high percentages of 96.9% and 86.7% were achieved, with and without including the side chains, respectively. The decrease is due to the inclusion of the nitrile group necessary for the Knoevenagel polymerization, which is not biosourced. For polymer bPPTzTz, the percentages were 96.3% and 66.7%, with and without the side chains, respectively. This result is expected, as the dithiooxamide required for forming the thiazolothiazole ring in the Ketcham reaction is not biosourced. These findings highlight the importance of considering both metrics. While the %BioT values for polymer bPPTzTz and polymer bCN-PPV are similar due to the longer side chains present in polymer bPPTzTz, the %BioC metric reveals a significant difference. Polymer bPPTzTz contains 20% fewer biosourced atoms than polymer bCN-PPV when the side chains are excluded.
Polymer | %BioT | %BioC |
---|---|---|
bPPV | 100 | 100 |
bCN-PPV | 96.9 | 86.7 |
bPPTzTz | 96.3 | 66.7 |
Polymer | Yield (%) | M n (kDa) | M w (kDa) | PDI | T d (°C) | T g (°C) |
---|---|---|---|---|---|---|
bPPV | 51 | 370 | 1300 | 3.5 | 395 | 80 |
bCN-PPV | 92 | 7 | 21 | 3.0 | 400 | 35 |
bPPTzTz | 90 | 12 | 16 | 1.3 | 370 | — |
The molecular weights of the polymers were determined using SEC analysis in 1,2,4-trichlorobenzene (TCB). Polymer bPPV shows a high Mn of 370 kDa and an Mw of 1300 kDa, resulting in a PDI of 3.5. Achieving a high molecular weight is often a problem in Gilch polymerization due to lack of solubility,41 but the polymer obtained remained soluble in THF, 2-MeTHF, CHCl3, and TCB.
For polymer bCN-PPV, synthesized via Knoevenagel condensation, the Mn was measured to be 7 kDa, and the Mw was 21 kDa, with a PDI of 3.0. These lower molecular weights align with literature reports and are likely due to side reactions such as the Thorpe–Ziegler condensation and Michael addition, which alter the monomer ratios and hinder polymer chain growth.32,33 Lastly, for polymer bPPTzTz, synthesized using the Ketcham polymerization, a Mn of 12 kDa and a Mw of 16 kDa were obtained, giving a PDI of 1.3. These results are consistent with previous results in the literature.19 However, the molecular weight was likely limited by poor solubility in N,N′-dimethylformamide (DMF), as the polymer precipitated during the reaction.
Thermogravimetric analysis (TGA) and differential scanning calorimetry (DSC) were performed on each of the polymers (see Table 2 and Fig. S1–S4, ESI†). Polymers bPPV, bCN-PPV, and bPPTzTz exhibited high thermal stability, with a 5% weight loss occurring at 395 °C, 400 °C, and 370 °C, respectively. DSC measurements were conducted on each sample at heating rates of 20 °C min−1 and 5 °C min−1 to scan for thermal transitions such as the glass transition temperature (Tg) and the temperature of fusion (Tf), respectively. Polymer bPPV showed a Tg of 80 °C, which is slightly higher than what is reported for similar polymer MEH-PPV that possesses a Tg of around 70 °C.42,43 This increase may be due to the high molecular weight of bPPV. Polymer bCN-PPV displayed a Tg of 35 °C, which is consistent with literature.44 Lastly, no thermal transitions were observed for polymer bPPTzTz. it is worth noting that, at slower scan rate (5 °C min−1), no thermal transition corresponding to the Tf was observed for the three samples.
1H NMR spectra of polymers bPPV,45bCN-PPV,46 and bPPTzTz47 (see Fig. 1 and Fig. S30–S32 in the ESI†) were analyzed and compared with similar reports in the literature.45–47 For polymer bPPV, the signal at 7.55 ppm corresponds to the vinylene protons, while the signal at 7.23 ppm corresponds to the benzylic protons. Signals at 4.00 ppm and in the range of 1.85 to 0.92 ppm are attributed to the ethylhexyl side chains. For polymer bCN-PPV, the multiplet at 8.1–7.7 ppm, which integrates for three protons, corresponds to two protons on the benzene ring and one proton from the alkene group. The multiplet at 7.1–6.8 ppm corresponds to two protons on the other benzene ring. Signals between 4.2–3.6 ppm and 1.9–0.6 ppm are assigned to the alkyl side chains. Notably, signals at 6.56 ppm and 3.24 ppm have been attributed to the cis-conformation of polymer bCN-PPV in previous reports.46 By integrating the signal at 3.24 ppm and comparing it to the signal at 4.2–3.6 ppm, the cis-conformation content was estimated to be approximately 8%. For polymer bPPTzTz, the signal at 10.5 ppm corresponds to residual aldehyde end groups. Signals in the 8.1–7.5 ppm region correspond to protons on the benzene ring, while signals at 4.13 ppm and 2.0–0.9 ppm are assigned to the alkyl side chains.
The analysis by FTIR spectroscopy provided key insights into the structural features of polymers bPPV,48bCN-PPV31 and bPPTzTz.47,49 As shown in Fig. 2, for polymer bPPV, signals in the region of 2800–3100 cm−1 correspond to sp2 and sp3 C–H bond stretching, with the signal at 3060 cm−1 attributed to the trans-vinyl C–H stretch. Signals around 1500–1350 cm−1 correspond to semicircular phenyl stretching and alkyl CH2 stretching. The signals at 1033 cm−1and 1195 cm−1 are assigned to C–O stretching of the alkyl–O bond and the phenyl–O bond, respectively. Signals at 856 cm−1and 969 cm−1 are attributed to out-of-plane wagging of the benzylic C–H and trans-vinyl C–H, respectively. For polymer bCN-PPV, signals in the 2800–3000 cm−1 region correspond to sp3 and sp2 C–H stretching. The signal at 2012 cm−1 corresponds to nitrile stretching, which is shifted to a lower wavenumber compared to the monomer (2250 cm−1) due to conjugation with the vinylene groups formed during polymerization. Signals around 1500–1350 cm−1 correspond to semicircular phenyl stretching and alkyl CH2 stretching. Signals at 1029 cm−1 and 1205 cm−1 are assigned to C–O stretching of the alkyl–O bond and the phenyl–O bond, respectively. For polymer bPPTzTz, sp3 and sp2 C–H stretching signals were observed between 2800–3000 cm−1. A signal at 1684 cm−1 likely corresponds to residual aldehyde end groups, which are expected under the polymerization conditions used. The signal at 1604 cm−1 could correspond to the CN stretching. Signals around 1400 cm−1 are assigned to C
C stretching vibrations within the aromatic ring. The signal at 1211 cm−1 corresponds to C–O stretching of the phenyl–O bond. Lastly, the signal at 1022 cm−1 is assigned to a combination of both the C–O alkyl stretching and the C–S stretching in the thiazolothiazole ring.
The optical and electrochemical properties are shown in Table 3, Fig. 3 and in Fig. S5–S15 (ESI†). For polymer bPPV, the UV-Vis analysis and cyclic voltametric analysis showed an λmaxsol at 510 nm and a slightly red-shifted λmax
film at 520 nm, with an Eg
optic of 2.1 eV and an Eg
elec of 2.3 eV. At an excitation wavelength of 450 nm, polymer bPPV exhibited an λF
max of 555 nm and a φfl of 0.49. The HOMO and LUMO energy levels were estimated to be −5.0 eV and −2.7 eV, respectively. We also determined the εmax to be 2.6 × 104 M−1 cm−1 and the αmax to be 15 × 104 cm−1. This is consistent with data found in literature.52–55 For polymer bCN-PPV, no shift in absorption maxima was observed between the solution and thin film spectra, both showing a λmax of 450 nm, with an Eg
optic of 2.3 eV and an Eg
elec of 2.3 eV. At an excitation wavelength of 425 nm, an λF
max of 555 nm was obtained, resulting in a large Stokes shift of 105 nm, and a φfl of 0.20. The HOMO and LUMO energy levels were −5.4 eV and −3.1 eV, respectively. We also determined the εmax to be 1.7 × 104 M−1 cm−1 and the αmax to be 9 × 104 cm−1.This is mostly consistent with data found in literature, however, we did not observe a reversibility peak, so this result should be interpreted with caution.52,53 It was noted that a lower φfl at 0.20 was obtained (0.35–0.4 in literature52,53), however it is hard to point to a specific explanation for this result as results found in literature typically have different side chains, molecular weight and/or methodology to obtain the φfl.52,53 For polymer bPPTzTz, an λmax
sol of 500 nm and a slightly red-shifted λmax
film at 510 nm were observed, with an Eg
optic of 2.0 eV and an Eg
elec of 2.1 eV. Notable shoulders appeared at 460 nm and 540 nm on either side of the absorption maximum in the UV-Vis spectra of polymer bPPTzTz, which can be attributed to transitions at different vibrational levels from the ground state to the excited state. This effect is more pronounced in the photoluminescence spectra, where an λF
max of 510 nm was obtained, with additional peaks at 470 nm and 550 nm, resulting from transitions from the excited state to the ground state at different vibrational levels. A φfl of 0.31 was obtained, and the HOMO and LUMO energy levels were −5.5 eV and −3.4 eV, respectively. We also determined the εmax to be 1.8 × 104 M−1 cm−1 and the αmax to be 8 × 104 cm−1. There aren’t precedents in the literature to compare the data obtained for bPPTzTz. Overall, the data highlight distinct optical and electrochemical characteristics for each polymer and show their potential for PLED applications.
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Fig. 3 (a) UV-Vis spectra in solution in CHCl3, (b) photoluminescence spectra in solution in CHCl3 and (c) UV-Vis spectra in thin films of polymers bPPV, bCN-PPV and bPPTzTz. |
Polymer |
λ
max![]() |
λ
max![]() |
λ
F![]() |
E
g![]() |
E
g![]() |
ε max | α max | HOMO | LUMO | φ fl |
---|---|---|---|---|---|---|---|---|---|---|
nm | nm | nm | eV | eV | 104 M−1 cm−1 | 104 cm−1 | eV | eV | — | |
a Absorption maxima in thin films. b Absorption maxima in solution in CHCl3. c Photoluminescence maxima in solution in CHCl3. d Optical band gap from the thin film spectra. e Electronical band gap. f Molar absorption coefficient in CHCl3. g Absorption coefficient in thin films. h Relative fluorescence quantum yield. | ||||||||||
bPPV | 520 | 510 | 555 | 2.1 | 2.3 | 2.6 | 15 | −5.0 | −2.7 | 0.49 |
bCN-PPV | 450 | 450 | 555 | 2.3 | 2.3 | 1.7 | 9 | −5.4 | −3.1 | 0.20 |
bPPTzTz | 510 | 500 | 510 | 2.0 | 2.1 | 1.8 | 8 | −5.5 | −3.4 | 0.31 |
The results highlight the potential of biosourced materials in reducing reliance on petroleum-based precursors while maintaining relevant properties for applications such as transistors and PLEDs. Notably, polymer bPPV achieved 100% biosourced atom content and suitable optical properties, while polymers bCN-PPV and bPPTzTz demonstrated high renewable atom percentages with distinct electronic and structural characteristics. These findings underline the feasibility of incorporating renewable resources and sustainable synthesis approaches in the development of advanced materials for organic electronics. Future efforts should focus on improving the renewability aspect of the reaction condition of the monomer synthesis (NaH, SOCl2, PCC, DMF, halogenated solvents…), as the chemical industry reduces its dependence on petroleum-based, toxic and/or dangerous chemicals, but it is still marking a significant step toward the creation of fully renewable organic electronic devices.
Footnote |
† Electronic supplementary information (ESI) available: Materials, full experimental details and characterisation. See DOI: https://doi.org/10.1039/d5nj00992h |
This journal is © The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2025 |