INTRODUCTION

The field of conductive polymers has recently attracted much attention from many researchers due to their potential in various applications, such as anti-static and anti-corrosion coating materials, batteries and supercapacitors, solar cells, sensors, light emitting diodes, and transparent electrode materials.1, 2, 3 Thiophene and dithienopyrrole are among the promising building blocks for the development of high-performance conjugated polymers for organic electronic devices because of their excellent planarity and strong electron-donating properties.4, 5, 6 Additionally, their fused-ring structure minimizes chain distortion, resulting in planarization of the polymer chain and improved 𝜋–𝜋 stacking. Furthermore, P3HT has been used as a model system for fundamental study due to its distinctive hair-rod structure, which comprises a hard conjugated backbone and flexible alkyl side chains that are effective for solubilization.7, 8

In recent years, the development of high-performance conjugated polymers by copolymerization has also shown promise. Copolymerization is widely used to develop novel conjugated polymers with physical and chemical properties that are distinct from and in between those of precursor homopolymers. However, a copolymer significantly differs from a composite and a blend. Jin . performed electropolymerization (EP) of styrene and pyrrole monomers and found that the product polymer was a copolymer of pyrrole and styrene instead of a composite or blend of polypyrrole and polystyrene. Copolymerization has recently been demonstrated to be capable of modifying the wavelength range of light absorption, frontier energy levels, and solubility of conjugated polymers.9, 10 Recently, Acker designed the novel N-anisylphenothiazine–bithiophene conjugated copolymer p(APT-T2), which could be a promising material to design an electrode for energy storage applications due to its intrinsic conductivity combined with the presence of defined redox centers.11 In 2020, Lin . designed six conjugated copolymers using thiophene as a fundamental unit, which all exhibited significantly improved electrochemical stability and noteworthy color changes when transitioning from the oxidized to neutral state with increasing conjugation length.12 In the same year, Zhen Xu and coworkers synthesized a novel copolymer PEM-11 via electrochemical copolymerization of two donor-acceptor type monomers, which exhibited stable n-doping, favorable cycle stability, and a lower electrochemical/optical band gap. The results suggested that the obtained copolymer could be a promising candidate for electrochromic windows, e-papers, or eyewear applications.13 Furthermore, in 2022, Hao Dong . reported a series of D-A copolymers with naphthodithiophene (NDT) as the electron donor (D) and benzodipyrrolidone (BDPP) as the electron acceptor (A). The four D-A copolymers showed excellent thermal stability, and the thermal decomposition temperature was above 380 °C.14

Moreover, another well-known technique for creating polymer films using an electric field is electrochemical polymerization, which is straightforward, fast, efficient, and cost-effective. In contrast to the conventional method, which requires harsh conditions (high temperature and inert environment) and can take several hours or days, the electropolymerization approach is highly effective for synthesizing polymer films because the reaction can be carried out under ambient conditions and in a matter of seconds or minutes. Additionally, the prepared films only formed on the electrodes without any obvious signs of a reaction in the solution. Moreover, the electropolymerization approach uses inexpensive supporting electrolytes instead of specialized catalysts and expensive complexants for solution-phase synthesis12, 15, 16. However, the choice of applied voltage in the electropolymerization process can significantly affect the growth rate and quality of the produced polymer. Higher applied voltages can lead to faster growth rates but lower quality films, while lower applied voltages can result in higher quality films but slower growth rates. Therefore, the applied voltage should be carefully considered balancing the growth rate and quality of the polymers.

In comparison to polydithienopyrrole, polythiophene has a better redox potential and is more affordable, making it a potentially useful material for optoelectronic applications.17 Nevertheless, due to their decreased backbone planarity and disordered molecule packing with irregularity restricting their application, the regio-random chemical structure of polythiophene and its derivatives has been found to only provide limited charge transfer in the solid state.18 Dithiopyrrole, on the other hand, has long been recognized for its distinct features, including exceptional thermal and electrical stability due to its broad HOMO-LUMO energy gap. Consequently, we attempted to use electrochemical copolymerization at various applied voltages to incorporate thiophene with dithienopyrrole units. Herein, thiophene and dithienopyrrole derivatives were used to prepare conjugated copolymers at three distinct applied voltages of 1.4, 1.435, and 1.6 V via the linear sweep voltammetry potentiostatic technique. The relationship between the electropolymerization conditions and the electrochemical properties of the conjugated copolymers was then studied in detail.

EXPERIMENTAL

RESULTS AND DISCUSSION

Electrochemical copolymerization of 3HT and HPDTP

Before conducting the electrochemical copolymerization to synthesize copolymers P1, P2, and P3, the onset oxidation potentials (E) of monomers 3HT and HPDTP were examined from their cyclic voltammograms (Figure 1).

The acquired current-time characteristic curves for the electrochemical copolymerizations to synthesize copolymers P1, P2, and P3 are shown in Figure 2.

After the electropolymerizations were performed successfully, the chemical structures of copolymers P1, P2, and P3 were characterized using FTIR spectroscopy, and the results are shown in Figure 3.

Optical properties of the copolymer P(3HT-random-HPDTP)

Next, the optical properties of the product copolymer were characterized using UV‒Vis absorption spectroscopy. The resulting chemical structure indicated that copolymers P1, P2, and P3 are the same compound. Therefore, copolymer P1 was used as a sample to analyze the optical properties of the prepared copolymer. The UV‒Vis absorption spectra of the copolymer and P(HPDTP) are shown and compared in Figure 4 to investigate the effect of the expanded - conjugated system on the optical properties of the synthesized copolymer.

Electrochemical properties of copolymer P(3HT-random-HPDTP)

By employing the cyclic voltammetry (CV) technique, the electrochemical behaviors of copolymers P1, P2, and P3 were investigated to better understand their electrochemical activity.

The results of the electrochemical behaviors of P1, P2 and P3 are presented in Figure 5.

DISCUSSION

Figure 1 demonstrates the E of the 3HT and HPDTP, which began at 1.4 and 0.8 V, respectively, and HPDTP also had oxidation peaks at 1.0 and 1.6 V. As a result, the applied voltage for electropolymerization should be above the E and under the overoxidation of both monomers, which ranges from 1.4 to 1.6 V. Consequently, copolymers P1, P2, and P3 were prepared by a linear sweep voltammetry potentiostatic technique with an applied voltage of 1.4 V (start point), 1.435 V (intersection point), and 1.6 V (endpoint).

As seen in Figure 2, the current intensities decrease gradually with increasing reaction time for all three electropolymerizations. The prepared conductive copolymers exhibited good electrochemical redox activity, as evidenced by the significant growth of the corresponding conductive copolymers on the ITO glass.

FTIR spectroscopy was scanned in the frequency region of 600-4000 cm at room temperature using an infrared spectrometer by employing the KBr pellet technique. The copolymers P1, P2, and P3 all have distinctive bands that are comparable, as seen in Figure 3 and Table 1. These bands extend from 725 to 850 cm, which are related to the C-H bending vibrations of the C-H linkage in the aromatic structure, and from 940 to 1125 cm, which are associated with the C-S stretching vibration of the thiophene structure. Furthermore, the typical bands of pyrrole structures’ C-N stretching lie in the range of 1230–1320 cm, whereas the –CH2 and -CH3 stretching and bending vibrations exhibit bands from 1440-1520 cm and 2810-2980 cm, respectively. According to the FTIR results, at applied voltages of 1.4, 1.435, and 1.6 V, electrochemical copolymerizations were effectively performed to produce copolymers P1, P2, and P3, which all have both monomers 3HT and HPDTP in their structures.

The optical properties of the copolymer are analyzed and shown in Figure 4. According to Figure 4, the copolymer exhibits broad wavelength absorption from 300 nm to 550 nm, which is longer than P(HPDTP), 350 nm to 550 nm. The longer wavelength absorption is due to the — excitation of the expanded -conjugation of the copolymer. Moreover, as the size increases, the copolymer intensity absorption is much larger than that of polymer P(HPDTP).

The energy bandgap, which can be identified using the UV‒Vis absorption spectrum, is another significant parameter for evaluating the optical characteristics of the conjugated copolymer. Using the Plank equation (Eg(opt) = 1240/λ), the calculated energy bandgap of the copolymer is 2.33 eV, which is larger than the value of P(HPDTP), 2.02 eV, because of the increased number of conjugated bonds in the copolymer’s structure. The outcome shows that the copolymer has a high optical bandgap value, which makes it advantageous for high-temperature optical devices such as LEDs, lasers, or solar cells.

According to Figure 5, copolymers P1 and P2 exhibited distinct redox peaks with hysteresis (potential drift) between the anodic and cathodic peak potentials, which may be ascribed to several factors, including local polymer chain rearrangement, slow mutual transformation of various electronic species, slow heterogeneous electron transfer, and electronic charging of the interfacial exchange at the polymer/solution and metal/polymer interfaces. These factors can cause slow and complex electrochemical reactions, which can lead to hysteresis between the anodic and cathodic peak potentials19. However, the redox activity of copolymer P3 demonstrated irreversible behavior at a scan rate of 5 mV/s, which was attributed to the molecular size of the copolymer. With a larger molecule size, copolymer P3 exhibited a lower diffusion rate than copolymers P1 and P2.20

Additionally, an empirical equation was used in conjunction with cyclic voltammetry to evaluate the HOMO and LUMO energy levels of the copolymers, and the results are shown in Table 2. The experimental E of copolymers P1, P2, and P3 exhibited upshifted values, gradually resulting in lower HOMO and LUMO energy levels of copolymers P1, P2, and P3. This difference can be explained by the conjugation chain length of the copolymers. Longer conjugation chain lengths result in lower HOMO and LUMO energy levels. This is because the longer conjugation length allows for more delocalization of the electrons, which results in a lower energy level for the HOMO and LUMO energy levels.12 These lower HOMO and LUMO energy levels indicate that increasing the applied potential can increase the chain length of the copolymer.

As illustrated in Figure 5, the stability of the three copolymers was also examined, with a total of three cycles performed. The redox activities of copolymers P1 and P2 were sustained at approximately 60% and 80%, respectively, after three cycles of scanning, indicating generally excellent redox activity. On the other hand, after three scanning cycles, the electrochemical stability of copolymer P3 reaches a stability of over 97%. This improved electrochemical stability was achieved by increasing the chain length of the copolymer, which benefits by raising the applied voltage of the electropolymerization of copolymer P3.

CONCLUSION

3HT-HPDTP random conjugated copolymers were effectively constructed at different applied voltages of 1.4, 1.435, and 1.6 V by electrochemical copolymerization using a linear sweep voltammetry potentiostatic technique. The structural, optical, and electrochemical properties of the prepared copolymers were then examined and compared. With an increase in the applied voltage during electropolymerization, the HOMO levels of copolymers P1, P2, and P3 gradually decrease. Moreover, the electrochemical stability of copolymer P3 was significantly improved, reaching above 97% when prepared at an applied voltage of 1.6 V. The preparation of high electrochemical stability copolymers for a variety of optoelectric applications using the linear sweep voltammetry potentiostatic technique has been demonstrated to be highly adaptable, straightforward, and effective.

ACKNOWLEDGMENT

This research was fully supported by the Vietnam National Foundation for Science and Technology Development (NAFOSTED) under grant number ‘‘104.02-2020.39”.

Abbreviations

Proton nuclear magnetic resonance (1H NMR), Fourier transform infrared (FT-IR) spectroscopies, gel permeation chromatography (GPC), deuterated chloroform (CDCl), 4-(4-hexylphenyl)-4H-dithieno[3,2-B:2’,3’d] pyrrole (HPDTP), cyclic voltammetry (CV).

Acknowledgments

This research was fully supported by the Vietnam National Foundation for Science and Technology Development (NAFOSTED) under grant number ‘‘104.02-2020.39”.

Author’s contributions

Thao Phuong Le Nguyen, Cam H. T. Nguyen and Ha Tran Nguyen conceptual the project methodology, wrote the original draft and supervised the investigation. Thao Thanh Bui, Bao Kim Doan, Tam Hoang Luu, Chau Duc Tran, Thuy Thu Truong, Tung Viet Tuan Tran, Hai Le Tran, Xuan Van Mai analysed experimental data. H. All authors discussed and edited the manuscript.

Competing interests

The authors declare that they have no competing interest.