Open Access Article
Kok Chan Chong
abc,
Kang Le Osmund Chin
ab,
Shi Jun Ang
d,
Ran Tao
ab,
Jianwei Xu
*a and
Ming Hui Chua
*ab
aInstitute of Sustainability for Chemicals, Energy and Environment (ISCE2), Agency for Science, Technology and Research (A*STAR), Singapore. 1 Pesek Road, Jurong Island, Singapore 627833, Republic of Singapore. E-mail: xu_jianwei@a-star.edu.sg; chua_ming_hui@a-star.edu.sg
bInstitute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A*STAR), Singapore. 2 Fusionopolis Way, Innovis, #08-03, Singapore 138634, Republic of Singapore
cFuture Energy Acceleration & Translation (FEAT), Strategic Research & Translational Thrust (SRTT), A*STAR Research Entities, 1 Fusionopolis Way, #20-10, Connexis North Tower, Singapore 138632, Republic of Singapore
dInstitute of High Performance Computing (IHPC), Agency for Science, Technology and Research (A*STAR), Singapore. 1 Fusionopolis Way, #16-16, Connexis North Tower, Singapore 138632, Republic of Singapore
First published on 14th April 2026
Thieno[3,4-c]pyrrole-4,6-dione (TPD) is a strong imide-based electron acceptor that remains under-explored for electrochromic (EC) conjugated polymers, with existing studies limited by narrow donor scope and the use of varying device structures, hindering systematic structure–property comparisons. Herein, a series of seven TPD-based donor–acceptor conjugated polymers incorporating thiophene-derived donors, terthiophene, quaterthiophene, pentathiophene, thieno[3,2-b]thiophene (TT), 3,4-ethylenedioxythiophene (EDOT), dithieno[3,2-b:2′,3′-d]pyrrole (DTP), and cyclopenta[1,2-b:5,4-b′]dithiophene (CPDT), are synthesised to elucidate the roles of conjugation length, backbone planarity, and donor strength in governing EC properties. Systematic modulation of donor structures enables tuning of neutral-state colours from grey to purple and dark blue, while oxidised states exhibit different grey hues. Stronger electron-donating units significantly enhance EC performance, with the EDOT-based polymer exhibiting the highest optical contrasts of 23.8% (595 nm) and 46.7% (1800 nm), while the DTP-based polymer shows the best open circuit memory retention (ca. 74% retention of initial transmittance after 10 minutes), fastest response times of 4.3 (bleaching at 608 nm) and 6.8 s (colouration at 1400 nm) and highest coloration efficiencies of 801.1 and 1358.5 cm2 C−1. Meanwhile, long-term switching stability appears to be more influenced by polymer molecular weight, with the pentathiophene-based polymer having the highest weight average molecular weight (Mw) of 104.5 kDa, demonstrating the highest durability, retaining 79.1% of its initial optical contrast after 3000 cycles. In addition, the electrofluorochromic (EFC) behaviour is observed for five polymers, with the terthiophene-based polymer showing the best contrasts of IOFF/ON 11.7 for fluorescence switching at 710 nm. Overall, this work establishes a comprehensive structure–property framework for TPD-based EC polymers, providing design rules that enable predictive tuning of colour, efficiency, and stability, and supporting the rational and potentially data-driven development of future high-performance EC materials.
Donor–acceptor (D–A) type conjugated polymers are widely studied for EC applications. They often exhibit robust EC switching performance, and offer tuneable optical properties such as EC switching colours via the rational selection of different aromatic electron-donor and electron-acceptor monomers. Common donors include thiophene-based monomers, triphenylamines, carbazoles, and pyrroles,7–12 while common acceptors include quinoxalines, benzothiadiazoles (BTD), and triazoles.13 Based on their different structures, and electron donating and withdrawing strengths, the selection and combination of monomers influence the polymers’ frontier molecular orbital energies, absorption profiles, as well as optical and electronic bandgaps,14–17 which may also have an effect on EC switching parameters, such as optical contrasts (OC), response times (τ), open circuit memory retention, colouration efficiencies (CE) and long-term switching stabilities. Based on this principle, numerous D–A type EC polymers bearing different acceptor groups have been developed over the years,13 with reported working colours spanning almost the entire colour palette.18,19 However, gaps still remain in the pursuit of precise colour tuning with the optimization of EC switching performance in the design of D–A type EC polymers. Future EC materials are expected to be increasingly tailored to application-specific requirements, guided by both expert intuition and emerging artificial intelligence and machine learning approaches.20,21 In this context, a comprehensive understanding of structure–property relationships, particularly across a broader range of monomer building blocks, is essential to enable predictive control over EC switching colours and performance to rationally guide materials development.
Imide and amide-based acceptors are widely used building blocks for low-bandgap conjugated polymers with efficient charge transport in optoelectronic applications, owing to their strong electron-withdrawing characteristics and versatile functionalisation, for example through the introduction of different side chains at the nitrogen positions to fine-tune polymer properties.22–25 Extensive studies have been carried out on EC polymers bearing diketopyrrolopyrrole,26–29 isoindigo,30–33 and rylene diimide34–36 acceptors. Our team has also studied EC conjugated polymers with bay-isoindigo,37 and pyromellitic diimide acceptors,38 as well as polymers featuring novel diimide-based acceptors prepared via inverse electron-demand Diels Alder or Diels Alder reactions between different diimide precursors and triazine or tetrazine.39–42 Polythiophenes are widely regarded as benchmark conjugated polymers due to their favourable photophysical and electronic properties for optoelectronic applications. Incorporation of thieno[3,4-c]pyrrole-4,6-dione (TPD) as an acceptor co-monomer provides an effective strategy to further tune these properties while largely preserving the planarity and rigidity of the polythiophene backbone. Conjugated polymers bearing a TPD acceptor have commonly been reported for photovoltaics43–45 and field effect transistor applications,46–49 and more recently, thermoelectrics50 and photocatalysis.51,52 Studies of TPD-based EC polymers are however limited, with only recent reports from Onal et al.,53 Song et al.,54 and Zhen et al.,55 confined to bearing one to two thiophene, 3,4-ethylenedioxythiophene (EDOT), or 3,4-propylene dioxythiophene (ProDOT) donors (Table S3, SI). More importantly, with the limited choice of donors and varying EC device (ECD) structures used in these reports, it may be difficult to get a clear picture of important structure–property relationships of TPD-based EC polymers, which is crucial to guide future materials development.
To fully realise the potential of TPD as a versatile building block for high-performance EC polymers with tuneable colour, comprehensive structure–property relationship studies are required. In this study, seven TPD-based conjugated polymers bearing different numbers and types of thiophene(-based) donors (Scheme 1), p(TPD2T-T), p(TPD2T-2T), p(TPD2T-3T), p(TPD2T-TT), p(TPD2T-EDOT), p(TPD2T-DTP), and p(TPD2T-CPDT), were synthesized and studied for their EC properties. The use of different donors actually leads to a significant variation in neutral state colours from brown to magenta, purple and dark blue, while the oxidised state colours reveal different hues of grey. EC switching studies reveal that all polymers exhibit comparable OCs at both visible and near-infrared (NIR) wavelengths, while differing markedly in τs, CEs, and open-circuit memory. Polymers p(TPD2T-EDOT) and p(TPD2T-DTP), respectively incorporating stronger donors 3,4-ethylenedioxythiophene (EDOT) and dithieno[3,2-b:2′,3′-d]pyrrole (DTP),56 deliver superior performance: p(TPD2T-EDOT) exhibits the largest OC of 46.7% at 1800 nm, while p(TPD2T-DTP) shows the fastest switching τs (4.3/0.7 s for colouration/bleaching at 608 nm), the highest CE (1358.5 cm2 C−1 at 1400 nm), and best open-circuit memory (retaining ca. 74% of its initial transmittance after 10 min). In contrast, p(TPD2T-3T), which has the highest weight-average molecular weight (Mw = 104.5 kDa), demonstrates the best long-term switching stability, retaining 79.1% of its initial OC after 3000 cycles. This polymer also exhibits the highest electrofluorochromic (EFC) switching contrast (IOFF/ON = 11.7 at 710 nm). Collectively, these results provide a comprehensive understanding of structure–property relationships in TPD-based EC polymers, addressing the current lack of systematic studies in this area.
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| Scheme 1 Chemical structures of TPD-based EC polymers p(TPD2T-T), p(TPD2T-2T), p(TPD2T-3T), p(TPD2T-TT), p(TPD2T-EDOT), p(TPD2T-DTP), and p(TPD2T-CPDT) studied in this work. | ||
1H and 13C NMR spectra were recorded in deuterated solvents using a Bruker AV400SB 400 MHz NMR spectrometer, with chemical shifts expressed in parts per million (ppm) relative to the TMS reference. High resolution electron spray ionization mass spectrometry (ESI) was performed using an Agilent LC-QTOF 6545B. Gel permeation chromatography (GPC) was performed in THF solutions using an Agilent 1260 Infinity II GPC/SEC system using polystyrene as the standard. UV-Vis-NIR absorption spectra of polymer solutions, and EC spectroelectrochemistry together with kinetic switching studies were recorded and performed using an Agilent Cary 5000 UV-Vis-NIR spectrophotometer. A PalmSens4 Potentiostat/Galvanostat was used to perform cyclic voltammetry (CV) and apply voltages for EC spectroelectrochemistry and kinetic switching studies. CV studies were performed in a three-electrode cell configuration with a glassy carbon working electrode, a Pt wire counter electrode and an Ag wire pseudo-reference electrode. Polymers were dissolved in 0.1 M TBAPF6 DCM solution for solution CV studies, whereas polymers were deposited over a glassy carbon working electrode and immersed into 0.1 M LiClO4 in acetonitrile electrolyte for thin-film CV studies. CV studies were performed at a scan rate of 50 mV s−1, and referenced against the ferrocene/ferrocenium (Fc/Fc+) redox couple. Fourier-transform infrared (FTIR) spectra of polymers were recorded using a Bruker Vertex 70 FTIR spectrometer. Colorimetric analysis was performed using a Hunterlab ColorQuest XE colorimeter. Thermal gravimetric analysis (TGA) and differential scanning calorimetry (DSC) were performed on a TA Instruments TGA Q500 and PDSC Q100, respectively. The thickness of spin-coated polymer films on ITO/glass substrates were measured via surface profilometry using a KLA Tencor P16 surface profiler. Scanning electron microscopy (SEM) was performed using a Hitachi SU8220 field emission SEM.
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1 v/v, filtered over 0.45 µm PVDF filter frit) was pipetted onto the ITO surface of one pre-cleaned substrate and spin-coated at 500 rpm for 30 s using a Laurell WS-400-LITE spin-coater. The substrate was allowed to stand on a hotplate at 80 °C for a minute. The excess edges on the spin-coated substrates were wiped off with a cotton bud to obtain a 2 × 2 cm active area. Meanwhile, 250 µL of gel electrolyte, prepared by stirring 0.512 g LiClO4, 6.65 mL of propylene carbonate, and 2.8 g of PMMA (Mw 120k g mol−1), was pipetted onto the ITO surface of another substrate over a 2 × 2 cm demarcated area blocked-out by double-sided tape, and allowed to stand for 15–20 minutes. The ECDs were then assembled by sandwiching the two substrates with 0.5 cm of uncontacted edges on each substrate for electrical contact.
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4 v/v) eluent was performed to isolate the product as a yellow solid (332 mg, 87% yield). 1H NMR (500 MHz, CDCl3, δ): 0.88–0.94 (m, 12H), 1.32–1.44 (m + s, 40H), 1.90 (t, J = 5.8 Hz, 2H), 3.64–3.75 (m, 4H), 7.16 (s, 2H), 7.47 (dd, J = 8.0 Hz, 0.8 Hz, 2H), 9.12 (d, J = 8.0 Hz, 2H). 13C NMR (100 MHz, CDCl3, δ): 10.7, 14.1, 23.03, 24.1, 24.9, 28.6, 30.5, 37.4, 44.1, 83.5, 84.0, 113.3, 113.6, 124.2, 128.7, 128.9, 134.3, 144.4, 168.1. HRMS (ESI, m/z): [M + H]+ calculated for C44H65B2N2O6, 739.5023; measured, 739.5026.
:
4 v/v) eluent was performed to isolate the product as a yellow solid (314 mg, 85% yield). 1H NMR (500 MHz, CDCl3, δ): 0.84–0.88 (m, 12 H), 1.23–1.34 (m, 64 H), 1.92 (m, J = 2H), 3.69 (d, J = 7.3 Hz, 4H), 4.27 (m, 4H), 4.34 (m, 4H), 6.37 (s, 2H), 7.24 (d, J = 1.5 Hz, 2H), 7.33 (dd, J = 8.5 Hz, 2.7 Hz, 2H), 9.12 (d, J = 8.5 Hz, 2H). 13C NMR (100 MHz, CDCl3, δ): 14.1, 22.7, 26.7, 29.3, 29.6, 29.7, 30.0, 31.8, 31.9, 36.5, 44.4, 64.4, 64.9, 99.2, 105.3, 117.8, 119.0, 120.2, 129.7, 131.7, 136.6, 139.5, 142.4, 145.3, 168.8. HRMS (ESI, m/z): [M]+ calculated for C68H98N2O6S2, 1103.6939; measured, 1103.6935.
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1 molar equivalence ratio at a monomer concentration of 10 M. The Pd(PPh3)4 catalyst (0.05 equivalence) was added and the reaction mixture thoroughly degassed by the freeze–pump–thaw method. The reaction mixture was allowed to stir at 100 °C for 24 h, and thereafter upon cooling down to room temperature, the reaction mixture was added dropwise into a large excess of methanol to precipitate out the crude product. The crude product was collected via simple filtration, dried and purified using a Soxhlet extractor setup first by washing with hot methanol, acetone and hexane, and then extracted with chloroform. The solvent was removed using a rotary evaporator and the polymer product was washed with methanol, collected via simple filtration, and finally dried using a vacuum oven.p(TPD2T-T) was synthesized via Stille polymerization between compound 3 and 2,5-bis(trimethylstannyl)thiophene to afford a shiny purple solid (98.0% yield). 1H NMR (500 MHz, CDCl3, δ): 0.85 (m, 12H), 1.11–1.59 (m, broad, 64H), 1.89 (broad, 2H), 3.74 (broad, 4H), 6.67 (broad, 2H), 7.05 (broad, 2H), 7.47 (broad, 2H), 9.04 (broad, 2H). GPC using PS in THF as a standard (Mn = 9017, Mw = 9 350, PDI = 1.037). FTIR (KBr): v (cm−1) = 2918 (s), 2849 (s), 1690 (m), 1607 (s), 1457 (m), 1112 (m), 790 (m).
p(TPD2T-2T) was synthesized via Stille polymerization between compound 3 and 5,5′-bis(trimethylstannyl)-2,2′-bithiophene to afford a shiny purple solid (93.0% yield). 1H NMR (500 MHz, CDCl3, δ): 0.86 (broad, 12H), 1.25 (broad, 64 H), 3.73 (broad, 4H), 6.06–6.66 (m, broad, 8H), 8.62 (m, broad, 2H). GPC using PS in THF as a standard (Mn = 12 145, Mw = 17
822, PDI = 1.467). FTIR (KBr): v (cm−1) = 2921 (s), 2851 (s), 1687 (s), 1607 (s), 1453 (m), 1358 (m), 1111 (m), 786 (m).
p(TPD2T-3T) was synthesized via Stille polymerization between compound 3 and 5,5′′-bis(trimethylstannyl)-2,2′:5′,2″-terthiophene to afford a shiny purple solid (14.0% yield). 1H NMR (500 MHz, CDCl3, δ): 0.86 (s, broad, 12H), 1.25 (broad, 64 H), 1.84 (broad, 2H), 3.67 (broad, 4H), 6.89 (m, broad, 6H), 7.56 (m, broad, 4H), 9.01 (m, broad, 2H). GPC using PS in THF as a standard (Mn = 54
295, Mw = 104 517, PDI = 1.925). FTIR (KBr): v (cm−1) = 2921 (s), 2850 (s), 1687 (m), 1607 (s), 1456 (m), 1111 (m), 783 (m).
p(TPD2T-TT) was synthesized via Stille polymerization between compound 3 and 2,5-bis(trimethylstannyl)thieno[3,2-b]thiophene to afford a shiny purple solid (99.0% yield). 1H NMR (500 MHz, CDCl3, δ): 0.84–0.88 (m, broad, 12H), 1.25 (broad, 64H), 4.02 (broad, 4H), 6.42 (broad, 4H), 7.47 (broad, 2H), 8.70 (broad, 2H). GPC using PS in THF as a standard (Mn = 13
546, Mw = 21 500, PDI = 1.587). FTIR (KBr): v (cm−1) = 2921 (s), 2852 (m), 1687 (m), 1607 (s), 1459 (m), 1112 (s), 801 (m).
p(TPD2T-EDOT) was synthesized via Stille polymerization between compound 3 and 5,7-bis(trimethylstannyl)-2,3-dihydrothieno[3,4-b][1,4]dioxine to afford a shiny blue solid (70.4% yield). 1H NMR (500 MHz, CDCl3, δ): 0.93–0.99 (broad, 12H), 1.37 (broad, 16H), 1.84 (broad, 2H), 3.70 (broad, 4H), 4.44 (broad, 4H), 7.05–7.17 (m, broad, 2H), 7.47 (m, broad, 2H), 9.03–9.09 (m, broad, 2H). GPC using PS in THF as a standard (Mn = 5 078, Mw = 9650, PDI = 1.784). FTIR (KBr): v (cm−1) = 2919 (m), 2854 (m), 1687 (s), 1604 (s), 1431 (s), 1351 (s), 1105 (s), 872 (m).
p(TPD2T-DTP) was synthesized via Stille polymerization of compound 3 and 4-dodecyl-2,6-bis(trimethyltin)-4H-dithieno[3,2-b:2′,3′-d]pyrrole to afford a shiny blue solid (90.0% yield). 1H NMR (500 MHz, CDCl3, δ): 0.86 (m, broad, 12H), 1.26 (m, broad, 64 H), 1.92 (broad, 2H), 3.70 (broad, 4H), 4.35–4.43 (m, 8H), 7.34 (m, broad, 2H), 7.47 (m, broad, 2H), 9.12 (broad, 2H). GPC using PS in THF as a standard (Mn = 6300, Mw = 10 632, PDI = 1.688). FTIR (KBr): v (cm−1) = 2921 (s), 2851 (s), 1687 (m), 1607 (s), 1450 (s), 1358 (s), 1114 (s), 1082 (s).
p(TPD2T-CPDT) was synthesized via Stille polymerization between compound 3 and 2,6-bis(trimethyltin)-4,4-bis(2-dodecylbenzo)-4H-cyclopenta[2,1-b:3,4-b′]dithiophene to afford a shiny purple solid (90.0% yield). 1H NMR (500 MHz, CDCl3, δ): 0.86 (m, broad, 12H), 1.26 (m, broad, 64 H), 1.92 (broad, 2H), 3.70 (broad, 4H), 4.35–4.43 (m, 8H), 7.34 (m, broad, 2H), 7.47 (m, broad, 2H), 9.12 (broad, 2H). GPC using PS in THF as a standard (Mn = 10 496, Mw = 19
442, PDI = 1.852). FTIR (KBr): v (cm−1) = 2921 (s), 2851 (s), 1687 (m), 1607 (s), 1450 (s), 1358 (s), 1114 (s), 1082 (s).
Due to the rigid, π-conjugated backbones and associated intermolecular aggregation, 1H NMR spectra of the seven polymers measured in both CDCl3 and toluene-d6 exhibit broadened signals characteristic of reduced chain mobility. In the aromatic region (δ ∼ 6.5–8.5 ppm), broad low-intensity resonances are assigned to protons of the thiophene/thiophene-based donors. In the downfield aliphatic region (δ ∼ 2.5–4.0 ppm), weak, broadened low-intensity signals correspond to the methine and methylene protons adjacent to the branching point of the 2-ethylhexyl substituent on the TPD unit, as well as the α- and β-methylene protons of alkyl chains/groups attached to electron-rich thiophene/thiophene-based donor units (e.g., EDOT and DTP). The upfield region (δ ∼ 0.5–2.0 ppm) is dominated by intense, broad resonances arising from the remaining methylene and terminal methyl protons of the dodecyl and 2-ethylhexyl side chains. FTIR spectra of all seven polymers consistently exhibit strong bands at ∼1670 and 1738 cm−1, attributed to the C
O stretching vibrations of the TPD acceptor units. Intense bands in the range of ∼2850–2960 cm−1 correspond to the aliphatic C–H stretching vibrations of the 2-ethylhexyl and dodecyl side chains. Additionally, weak bands at ∼3065–3070 cm−1 are observed and assigned to aromatic C–H stretching of the thiophene-based units. Thermogravimetric analysis (TGA) of the seven polymers also shows that the polymers show considerable thermal stability with decomposition temperatures (at which 5% weight loss occurs) between 230.68 and 415.13 °C.
818 to 35
219 and 40
118 M−1 cm−1. The largest ε registered for p(TPD2T-3T) amongst the seven polymers could also be due to its exceptionally high Mw. Meanwhile, replacing a thiophene in each repeating unit of p(TPD2T-T) with thiophene-based donors thieno[3,2-b]thiophene (TT), EDOT, DTP, and cyclopenta[1,2-b:5,4-b′]dithiophene (CPDT), led to significant red-shift in λabs for p(TPD2T-TT), p(TPD2T-EDOT), p(TPD2T-DTP), and p(TPD2T-CPDT), at 520, 537, 565, and 558 nm, respectively. p(TPD2T-DTP) exhibits the most red-shifted absorption profile, which can be attributed to the strong electron-donating characteristic of the DTP unit and its ability to enhance intramolecular charge transfer (ICT) with the TPD acceptor, thereby reducing the bandgap. λabs of polymers p(TPD2T-T), p(TPD2T-2T), p(TPD2T-TT), and p(TPD2T-CPDT) in thin films were either comparable or slightly blue-shifted compared to that in solutions, whereas the thin film λabs of polymers p(TPD2T-3T), p(TPD2T-EDOT) and p(TPD2T-DTP) showed obvious red-shifting (Table 1 and Fig. 3).
| Polymer | λSolnabs a (nm) |
εb (M−1 cm−1) | λSolnonset c (nm) |
EOptg d (eV) |
λFilmabs e (nm) |
λSolnPL f (nm) |
λFilmPL g (nm) |
EOxOnset h (V) |
EHOMOi (eV) | ELUMOj (eV) |
|---|---|---|---|---|---|---|---|---|---|---|
| a Absorption maximum wavelength in chloroform solution.b Molar extinction coefficient.c Absorption onset wavelength.d Optical bandgap = 1240/λSolnonset.e Absorption maximum wavelength of the thin film.f Photoluminescence maximum wavelength in chloroform solution.g Photoluminescence maximum wavelength of the thin film.h Oxidation onset potential determined by solution CV, vs. Fc/Fc+.i HOMO energy level = EOxOnset – (−4.8) eV.j LUMO energy level = EHOMO + EOptg. | ||||||||||
| p(TPD2T-T) | 510, 624 (sh) | 30 818 |
700 | 1.77 | 492 | 604 | 710 | 0.97 | −5.77 | −4.00 |
| p(TPD2T-2T) | 494 | 35 219 |
693 | 1.79 | 490 | 608 | 708 | 0.79 | −5.59 | −3.80 |
| p(TPD2T-3T) | 498 | 40 118 |
697 | 1.78 | 520 | 602 | 697 | 0.55 | −5.35 | −3.57 |
| p(TPD2T-TT) | 520, 658 (sh) | 30 413 |
693 | 1.79 | 497 | 610 | 710 | 0.85 | −5.65 | −3.86 |
| p(TPD2T-EDOT) | 537 | 22 159 |
747 | 1.66 | 595 | 625 | — | 0.59 | −5.39 | −3.73 |
| p(TPD2T-DTP) | 565 | 34 218 |
780 | 1.59 | 608 | 655 | — | 0.42 | −5.22 | −3.63 |
| p(TPD2T-CPDT) | 558 | 36 289 |
685 | 1.81 | 555 | 666 | 715 | 0.52 | −5.32 | −3.51 |
Based on the absorption spectra onsets, the seven TPD polymers were determined to have rather low optical bandgaps (Eg) between 1.66 and 1.81 eV. Increasing the number of thiophene per repeating unit from 3 to 4 and 5, as well as the introduction of the TT donor did not result in remarkable differences in Eg amongst p(TPD2T-T), p(TPD2T-2T), p(TPD2T-3T) and p(TPD2T-TT), respectively. As compared to p(TPD2T-T), the introduction of stronger EDOT and DTP donors led to marked reduction in Eg for p(TPD2T-EDOT) and p(TPD2T-DTP) (1.77 vs. 1.66 vs. 1.59 eV, respectively). Meanwhile, with the CPDT donor, the Eg of p(TPD2T-CPDT) was slightly increased to 1.81 eV. The HOMO energy levels (EHOMO) of the polymers, as determined by cyclic voltammetry (Fig. S1, SI), were found to be correlate well with the strength of the thiophene-based donors, with polymer p(TPD2T-DTP) having the highest EHOMO of −5.22 eV and the lowest oxidation potential of 0.42 eV. This is consistent with DTP being the most electron-rich donor amongst those present in the seven polymers, which is often used to design low band-gap conjugated polymers exhibiting similar characteristics.56 Meanwhile, the LUMO energy levels (ELUMO) of the seven polymers were determined and found to be in the range between −3.51 and −4.00 eV (Table 1).
All seven polymers exhibit deep-red fluorescence in solutions, with photoluminescence (PL) maximum wavelengths (λPL) ranging between 604 and 666 nm (Fig. 1b). Polymers p(TPD2T-T), p(TPD2T-2T), p(TPD2T-3T), and p(TPD2T-TT) have fairly comparable fluorescence profiles whereas the introduction of EDOT, DTP, and CPDT donors markedly red-shifted the fluorescence spectra of p(TPD2T-EDOT), p(TPD2T-DTP), and p(TPD2T-CPDT), leading to λPL values of 625, 655, and 666 nm, respectively (vs. 604 nm for p(TPD2T-T)). Thin films of p(TPD2T-EDOT) and p(TPD2T-DTP) appear non-fluorescent, while the thin film fluorescence of the remaining polymers were red-shifted compared to that in the corresponding solutions (Fig. S3, SI). The red-shift in fluorescence could be attributed to stronger intermolecular π–π stacking between polymer chains in thin films, which causes greater structural planarity in the polymer backbones and enhances electron delocalization, thus effectively reducing emission energy.57 As such, p(TPD2T-CPDT), which is structurally more rigid and planar in solution due to the CPDT donor, experiences only a small redshift in λPL of 49 nm in the thin film, while p(TPD2T-T) being less rigid and planar in solution, experiences only a greater redshift in λPL of 106 nm in the thin film.
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| Fig. 2 DFT calculated HOMOs and LUMOs and their respective energies (MN15/def2-SVP) of one repeating unit of the TPD polymers (structures shown in the figure) studied in this work. | ||
The DFT-calculated HOMOs and LUMOs of the seven structures display relatively uniform electron-density distributions along the oligo-thiophene backbones, indicative of delocalized π and π* frontier orbitals. This delocalization is expected to facilitate intrachain charge transport upon electrochemical doping, thus is beneficial for efficient EC switching in the corresponding polymers.63 The calculated HOMO and LUMO energies for the repeating units agree with the trend of EHOMO and ELUMO of the seven polymers (Table 1). This includes modest reduction of the calculated HOMO–LUMO energy gaps from TPD2T-T to TPD2T-2T and TPD2T-3T. Meanwhile, replacing a thiophene unit with TT, slightly extending π-conjugation, resulted in a slightly higher HOMO and lower LUMO for TPD2T-TT relative to TPD2T-T. Substituting a thiophene unit with stronger EDOT, DTP, and CPDT donors gave higher HOMO energies in TPD2T-EDOT, TPD2T-DTP, and TPD2T-CPDT, with TPD2T-DTP having the highest calculated HOMO energy of −6.807 eV (vs. −7.304 eV of TPD2T-T). All computations were carried out with ORCA 6.1.1.64
While the absorption spectra of the seven polymers did not show noticeable changes on the application of increasing negative voltages, they exhibit gradual changes with increasing positive voltages, as shown in Fig. 3a–g, revealing the anodically-colouring nature of these TPD-based conjugated polymers. The respective changes in absorption spectra are due to the formation of polarons and bipolarons when the polymers undergo electro-oxidation. In the neutral state, the polymers show an intense absorption band with λabs between 490 and 612 nm in the visible region, and a low intensity and broad absorption band stretching into the NIR region, likely arising from strong intermolecular π–π interactions, excitonic coupling and charge-transfer states in the solid thin film state. Increasing applied voltages to a polymer generally led to the gradual collapse of its visible absorption band, accompanied by the emergence of a far-red absorption band and another broader NIR absorption band. For the polymers p(TPD2T-T), p(TPD2T-2T) and p(TPD2T-3T), changes in the absorption spectra occur from ca. +1.0 to +1.2 V. The incremental absorption changes for the three polymers appear to taper off at +2.2, +2.2, and +2.0 V, respectively. Beyond this point, distinctly new absorption profiles with λabs ranging from ca. 420 to 375 nm emerge as applied voltages increase. Going from p(TPD2T-T) to p(TPD2T-2T) and p(TPD2T-3T), the intensities of newly-emerged NIR absorption bands increase relative to the absorbance in the visible regions (at 492, 490, and 518 nm, respectively) in the oxidised states (Fig. 3a–c). Likewise, the p(TPD2T-TT) polymer showed incremental spectral changes from +1.0 V until +2.2 V, where the absorption intensities at both 525 and 1235 are somewhat comparable (Fig. 3d).
Meanwhile, with the introduction of stronger donors, EDOT and DTP, the onset of absorption spectral changes for the p(TPD2T-EDOT) and p(TPD2T-DTP) polymers occurred much earlier at +0.4 and +0.2 V, respectively. The respective single neutral state absorption band at λabs of 596 and 612 nm gradually collapsed with increasing applied voltages, transitioning into a new far-red absorption band at λabs at 830 and 755 nm, respectively. This transition was accompanied by another broader new NIR absorption band at λabs of ca. 1825 and 1400 nm, respectively, with comparable intensities (Fig. 3e and f). This transition appears to taper off at ca. +1.5 V for p(TPD2T-DTP), after which the NIR absorbance at 1400 nm continues to rise until +2.0 V before dropping, while the far-red absorbance at 755 nm starts to reduce. For polymer p(TPD2T-CPDT), absorption spectra change occurs starting from +0.8 V. At +1.6 V, the electro-oxidised polymer shows three distinct absorption bands at λabs ca. 470, 800, and 1450 nm (Fig. 3g). Further increasing the applied voltages led to a decrease in the far-red and NIR absorbance, accompanied by an increase in the blue absorbance at ca. 450 nm.
In the neutral state, the polymers revealed a range of colours from light grey to brown, magenta brown, and reddish brown for p(TPD2T-T), p(TPD2T-2T), p(TPD2T-3T), and p(TPD2T-TT), respectively, as well as greyish blue, dark blue, and purple for polymers with stronger donors, p(TPD2T-EDOT), p(TPD2T-DTP), and p(TPD2T-CPDT), respectively. The corresponding colour changes for polymers p(TPD2T-T), p(TPD2T-2T), p(TPD2T-3T), p(TPD2T-TT), p(TPD2T-EDOT), p(TPD2T-DTP), and p(TPD2T-CPDT) upon electro-oxidation (at +2.2, +2.2, +2.0 V, +2.0, +1.5, and +1.6 V) are shown in Fig. 3h. Overall, all seven polymers exhibit grey colours of different hues in the oxidised state.
In the neutral state, a general decrease in L* is observed from p(TPD2T-T) to p(TPD2T-2T), p(TPD2T-TT) and p(TPD2T-3T), indicating progressively darker colours with increasing conjugation length of the oligothiophene donors. The introduction of stronger EDOT, DTP and CPDT donors, led to more drastic reduction in L* for p(TPD2T-EDOT), p(TPD2T-DTP), and p(TPD2T-CPDT) with respectively. Upon electro-oxidation, all polymers show an increase in L*, corresponding to lighter colour and greater transmissivity. The magnitude of this change (ΔL*) generally increases with donor strength, with p(TPD2T-DTP) exhibiting the largest ΔL* (+10.43), while p(TPD2T-T) shows only a minimal change (+0.53). It is noted that absolute L* values may also be influenced by variations in film thickness (Table S2), although not significantly. For example, p(TPD2T-CPDT) has a thinnest film of 59.2 nm thickness but also the darkest neutral colour (L* = 76.67), whereas p(TPD2T-TT) has the thickest film of 226.8 nm thickness, but the third lightest neutral colour (L* = 86.19).
Analysis of the a* coordinate reveals that most polymers exhibit positive values in the neutral state, indicating a red component that increases from p(TPD2T-T) to p(TPD2T-TT), in line with increasing effective conjugation in the donor. However, incorporation of stronger donors leads to a reduction in a* that appears to correlate with donor strength (CPDT < EDOT < DTP), with p(TPD2T-DTP) displaying negative values, indicative of a shift towards greenish-blue hues. A clearer trend is observed in the b* coordinate. While polymers with weaker donors (T, 2T, TT) show small positive or near-zero b* values (slightly yellowish), increasing conjugation (3T, CPDT), and especially stronger donors (CPDT, EDOT, DTP) result in increasingly negative b* values, corresponding to more pronounced blue colouration. This is consistent with the red-shifted absorption profiles observed for these systems.
In the oxidised state, the colour coordinates converge towards “true black” (a* = 0, b* = 0) (Fig. S6, SI), giving rise to greyish hues across all seven polymers. Compared to the neutral state, polymers with weaker donors show smaller magnitude decreases in b* (become bluer) upon oxidation, whereas those with stronger donors (EDOT, DTP, CPDT) exhibit larger magnitude increases in b* (become yellower), with p(TPD2T-DTP) displaying the largest change (Δb* = +12.39). Meanwhile, increasing the extent of donor's conjugation from T to 2T, TT, and 3T increases the magnitude of change in a* as oxidised polymers become less red (Δb* = −1.72, −4.46, −8.61, and −10.56, respectively). Polymers with stronger donors appear to have smaller Δb* with p(TPD2T-DTP) having a Δb* of +0.28 instead.
The above trends are closely related to the polymers’ switching τs (Table S2, SI), where τox and τre denote the times required for electro-oxidation and recovery, respectively. All seven polymers exhibit shorter τre than τox at both visible and NIR wavelengths while switching at NIR wavelengths is generally slightly slower than at visible wavelengths. Polymers incorporating stronger donors show faster switching. (TPD2T-EDOT) and p(TPE2T-DTP) exhibit relatively shorter τox/τre of 9.0/1.7 s and 4.3/0.7 s, respectively, for visible EC switching, and 11.9/1.3 and 6.8/1.2 s, respectively, for NIR EC switching. The faster switching of these polymers enable more complete EC transitions within shorter Δt, thereby allowing them to retain higher OCs under rapid switching conditions.
The colouration efficiency (CE) of the seven polymers was measured. Amongst them, p(TPD2T-EDOT) and p(TPD2T-DTP) exhibited exceptionally high CEs of 720.7 and 801.1 cm2 cm−1 for EC switching at 595 and 608 nm, respectively, and excellent CEs of 1012.1 and 1358.5 cm2 cm−1 for that in 1800 and 1400 nm, respectively. Comparatively, the other polymers show relatively lower CEs of 207 to 377 cm2 cm−1 for visible EC switching, and 200 to 630 cm2 cm−1 for NIR EC switching.
Open-circuit memory retention was evaluated at both visible and NIR wavelengths to assess the ability of the polymers to maintain their coloured (charged) states after removal of the applied potential. The transmittance of fully oxidised electrochromic devices (ECDs) was monitored over 10 min under open-circuit conditions. All polymers exhibit some degree of transmittance decay, indicating partial loss of the charged state over time (Fig. S7, SI). However, the extent of retention correlates strongly with donor strength. p(TPD2T-DTP) shows the best memory performance, retaining 75.4% and 73.2% of its initial transmittance at visible and NIR wavelengths, respectively, after 10 min. This is followed by p(TPD2T-EDOT), which retains 67.9% (visible) and 49.6% (NIR). In contrast, polymers bearing weaker donors, such as p(TPD2T-T) and p(TPD2T-TT), exhibit significantly poorer retention, maintaining only 19.7% and 16.5% (visible) and 19.2% and 22.1% (NIR), respectively.
The EC switching performance of the seven polymers reveals a clear structure–property relationship governed primarily by donor strength. The superior performance of p(TPD2T-EDOT) and p(TPD2T-DTP) in terms of OC, τ, CE, and open-circuit memory retention can be attributed to the strong electron-donating characteristic of EDOT and DTP, which enhances donor–acceptor interactions, lowers the bandgaps and oxidation potentials, and facilitates more efficient charge injection and extraction. This also promotes greater π-electron delocalisation along the polymer backbone, thereby stabilising oxidised polaronic and bipolaronic states. As a result, these polymers exhibit larger optical modulation, faster switching kinetics, higher optical modulation per injected charge,65–67 and slower charge recombination under open-circuit conditions. In contrast, secondary factors such as conjugation length (T to 3T) and structural rigidity (TT and CPDT) mainly influence optical absorption and colour tuning through bandgap modulation and improved backbone planarity, but exert a less pronounced effect on switching kinetics within this polymer series. We also acknowledge that the relatively smoother film morphologies of p(TPD2T-EDOT) and p(TPD2T-DTP) might have also contributed to these stellar performances (Fig. S4, SI). Meanwhile, the polymer's Mw does not appear to have any influence.
The long-term EC switching stability of the p(TPD2T-3T), p(TPD2T-EDOT) and p(TPD2T-DTP) polymers at their respective NIR wavelengths of study was further assessed by monitoring the transmittance at 1256, 1800, and 1400 nm, respectively, over 3000 cycles while switching at ±1.8 V, at a Δt of 20 s (Fig. S8, SI). Both polymers p(TPD2T-3T) and p(TPD2T-EDOT) exhibited relatively gradual changes in OCs indicating good durability. They experienced 10.7 and 15.1% loss to their initial OCs after 1000 cycles, respectively, which increased to 20.9 and 24.8% loss, respectively, after 3000 cycles. The relatively high molecular weight of p(TPD2T-3T) could have contributed to its robust cycling stability by creating physical entanglements that provide exceptional mechanical resilience and long-term cycling stability,68 whilst the electron-rich EDOT units in p(TPD2T-EDOT) significantly lower the operating oxidation potential and stabilize oxidized states through resonance delocalization and a more favourable oxidation profile.69 On the other hand, p(TPD2T-DTP) showed a more pronounced decrease in OC, losing 35.6% of its initial OC after 1000 cycles, and retaining 51.5% of the initial OC after 3000 cycles. This poorer stability may reflect the greater susceptibility of p(TPD2T-DTP) to over-oxidation, consistent with it having the highest HOMO level and lowest oxidation onset potential among the seven polymers (Table 1).
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| Fig. 5 EFC spectroelectrochemistry studies of polymers (a) p(TPD2T-T), (b) p(TPD2T-2T), (c) p(TPD2T-3T), (d) p(TPD2T-TT), and (e) p(TPD2T-CPDT). | ||
Structurally, this work expands the scope of donors for TPD-based EC polymers compared to existing work, with the inclusion of other thiophene-based donors such as TT, DTP, and CPDT. As shown in Table S3 (SI), all seven polymers show comparable Eg to those reported by Onal et al. and Song et al. Through the use of four and five thiophenes, as well as TT donors, we are also able to achieve brown neutral colouration not reported in prior work. Meanwhile, the greyish colourations of our TPD polymers in the charged state are consistent with those of previously reported work. The OCs obtained for our polymers were in the range of 17.5–23.8% for EC switching in the visible wavelength region, and 20.2–46.4% for EC switching in the NIR wavelength region, which are comparable to prior art (18–52%). Meanwhile, the τox of our polymers are slightly longer than those reported while the CEs of our polymers are comparable to those reported, although those of p(TPD2T-EDOT) and p(TPD2T-DTP) (1012.1 and 1358.5 cm2 C−1, respectively) were the highest recorded for TPD-based EC polymers thus far.
For long-term switching stability, our work has demonstrated that p(TPD2T-3T) and p(TPD2T-EDOT) can exhibit considerable stability up to 3000 cycles with 20.9 and 24.8% loss in initial OCs. This is significantly higher than the 200 cycles with 20% drop in OC reported by Song et al. While these results may be considered comparable to some other simple D–A type polymers, such as benzimidazole-EDOT73 and isoindigo-EDOT32-based polymers retaining 76 and 92% of electroactivity after 4000 switching cycles, respectively, they are still modest compared to some recently reported multi-donor D–A type conjugated polymers, such as the quinacridone-CPDT-ProDOT copolymer reported by Li et al.,74 and a black-to-transmissive BTD-fluorene-ProDOT copolymer reported by Chen et al.75 which retained 88.4 and 99% of their initial OCs after 100
000 and 126
000 cycles, respectively.
Finally, thin film ECD λPL values of the five polymers studied herein (697–715 nm) are more red-shifted than that of the TPD-ProDOT polymer reported by Song et al. (672 nm), with the IOFF/ON contrast for p(TPD2T-3T) of 11.7 comparable to that of the reported polymer (IOFF/ON 12.9).54
However, it is worth noting that the ECD structures differ between our work and that of prior arts, as our work fabricated sandwich type full-cell thin film devices with a polymer gel electrolyte, whilst Onal et al. and Zhen et al. adopted hall-cell ECDs, and Song et al., a “liquid-based” full cell device. Hence, EC and EFC switching parameters such as OCs and response times may not be directly comparable across the different studies.
Overall, this work demonstrates the effective tuning of colours and EC properties of TPD-based conjugated polymers through systematic donor engineering. The findings provide important structure–property insights, well addressing the current scarcity of comprehensive studies on TPD-based EC systems. These critical findings will be useful to guide the development of high performance EC and EFC materials with tuneable switching characteristics tailored to the functional needs of different end applications, such as smart windows for energy-saving, user-comfort and aesthetics in green buildings and automobiles. Furthermore, given the broad applicability of TPD-based conjugated polymers in other applications such as photovoltaics, field effect transistors, and thermoelectrics, as reported, this work may guide the development of multi-functional TPD-based EC conjugated polymers for advanced uses in a sustainable urban environment for greater energy-efficiency.78 With different combinations of donor and acceptor building blocks explored thus far in the development of EC and EFC conjugated polymers, there will also be opportunities to leverage on artificial intelligence and machine learning in future EC polymer materials design.
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