Retracted Article: A novel concept and design for highly efficient photoelectrocatalytic materials with high performance, stability, and charge transport properties: development of an innovative next-generation green technology

Abstract

In semiconductors, generating charges via catalysis is a highly challenging task and characteristic of heterojunction photoanodes. A dithiophene-4,8-dione spin-coated film layer has a positive effect on the holes (positive charge carriers) for a long time in BHJ films in the solid state of materials. The photoexcited holes created in the BHJ film can persist for long periods of time, which is beneficial for catalytic reactions. In this study, a photoanode is electrically coupled to a hydrogen gas-evolving platinum cathode. When the photoanode is electrically coupled to a H₂ gas evolving Pt cathode, curiously long-lived hole polaron states are observed on the timescale of seconds under operational conditions. These long-lived holes play a crucial role in enhancing the hydrogen peroxide oxidation performance of the film overlayer spin-coated onto the photoanode. The spin-coated film overlayer on the photoanode achieves the best oxidation performance for hydrogen peroxide of approximately 6.5 mA cm⁻² at 1.23 V_RHE without the need of a catalyst. This demonstrates the effectiveness of the overlayer in improving the catalytic performance of the photoanode with a better efficiency of 17.5% when using 851 nm excitation. This indicates that a relatively high percentage of incident photons at that specific wavelength is converted into photocurrent by the photoanode. This approach can lead to more efficient oxidation catalysis as demonstrated in the case of hydrogen peroxide oxidation.

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Introduction

By integrating solar-driven fuel synthesis with photovoltaic (PV) technologies, excess electricity generated during periods of high solar irradiation can be utilized for fuel production. The produced fuels can then be stored and used later, including during periods of low sunlight or high electricity demands. Solar-driven fuel synthesis offers a promising solution for the effective utilization of intermittently generated solar energy, addressing the challenge of energy storage and providing a more reliable and sustainable energy system. It can contribute to the development of a green and renewable energy for economy by providing a means for the conversion and storage of solar energy in the form of chemical fuels.¹ The production of green hydrogen via photoelectrochemical water splitting has gained considerable interest owing to the environmental benefits it offers on a commercial scale. Hydrogen generated from renewable sources can serve as a clean and sustainable fuel, with applications in various sectors, such as transportation, industry, and energy storage. As research and development in photoelectrochemical overall water splitting continue, efforts are made towards improving the efficiency and stability of photoelectrodes, exploring new materials, and optimizing system designs to achieve cost-effective and scalable solar-driven synthesis of green hydrogen gas production.² Furthermore, semiconductors offer the possibility of molecular engineering and synthesis of new materials with improved properties. Researchers can design and modify the chemical structure of materials to enhance their stability, charge carrier mobility, and catalytic activity, addressing the challenges associated with semiconductors, such as limited stability and lower charge carrier mobility compared to inorganic materials. The development of stable and efficient semiconductors designed for numerous photoelectrochemical applications is an active area of research. Ongoing efforts focus on designing new materials, optimizing device architectures, improving charge transport properties, and enhancing the overall performance and stability of photoelectrochemical devices.^3–5 Overall, the recent advances in OPV device efficiency have gained interest in leveraging semiconductors for various photoelectrochemical applications, paving the way for more sustainable and efficient solar-driven fuel synthesis of composite materials.⁶ Overall, BHJ architectures based on polymer donors and small molecular acceptors offer a promising difference to metal oxide semiconductors in devices. Their wide absorption range, tunability, and compatibility with low-cost fabrication methods make them attractive for efficient solar energy conversion, including photoelectrochemical full water splitting, and hold significant potential for the development of sustainable and scalable solar-driven fuel synthesis technologies in the near future.⁷ The short lifetime of photogenerated charges in semiconductors causes difficulties in achieving efficient charge separation, transport, and transfer to the electrolyte interface. Rapid charge recombination and trapping processes can limit the overall efficiency of charge transfer and utilization for photocatalytic reactions in PEC systems. To overcome these challenges, ongoing research efforts focus on developing strategies to prolong the lifetime of photogenerated charges and enhance charge transport and transfer kinetics in semiconductors. This includes exploring new materials, interface engineering, and device architectures that minimize charge recombination and improve charge extraction to achieve more efficient and stable photoelectrochemical systems. Addressing the kinetic challenge of short lifetime of photogenerated charges in semiconductors is crucial for advancing the field and realizing their full potential for efficient solar-driven fuel synthesis by photoelectrochemical systems.^8,9 Cobalt nanocatalysts are used for the purpose of boosting up the fuel-cell metal–air batteries. Doping with Co can lead to significant improvements in the electronic properties and structure of a catalyst, making it exhibit enhanced kinetics of the hydrogen evolution reaction, especially in alkaline media. This aligns with the broader efforts to develop efficient and cost-effective catalysts for renewable hydrogen production through electrocatalysis. It may be that nanoparticle suspensions can allow more penetration into the semiconductor, enabling the generation of long-lived charges and the electrolyte to have further effect on the charge carrier performance of materials and photoelectrodes, in addition to control of the hydrophilicity of the material surfaces. Another novel report on Fe-DAs/NC with Fe₂–N₆ further investigated fully oxygen reduction reaction (ORR) electrocatalysts in alkaline media. The (photo)electrochemical hydrogen gas production helps direct electrochemical hydrogenation with ∼58% conversion; overall, it has been observed by using ascorbic acid.^10–13 Charge carrier dynamics has been extensively conducted in photovoltaics (PVs) and, more recently, in polymeric photocatalysts in suspension, and investigations into charge carrier dynamics in photoelectrodes have been relatively limited thus far. Understanding the fundamental charge carrier dynamics in these systems is crucial for optimizing their performance and identifying potential limitations. Characterizing charge carrier dynamics involves studying processes such as charge generation, separation, recombination, and transport within photoelectrodes. This information can provide insights into the factors that influence the efficiency and stability of charge transfer processes in photoelectrochemical devices. By gaining a deeper understanding of charge carrier dynamics, researchers can identify strategies to improve the performance of photoelectrodes for efficient solar energy conversion.¹⁴ As the field of photo-electrochemistry continues to grow, it is expected that there will be increasing research efforts focused on investigating charge carrier dynamics in photoelectrodes. Such studies will provide valuable insights into the underlying mechanisms and enable the development of more efficient and stable systems for solar-driven fuel synthesis and photoelectrochemistry.^15,16 Here the improved operational stability underwater indicates the potential of the spin-coated film overlayer in mitigating the detrimental effects of the aqueous environment on the BHJ-based photoanodes. Water can induce degradation and hinder charge transport, making stability an essential consideration for practical applications. Overall, the utilization of a spin-coated film overlayer in BHJ-based photoanodes demonstrates the potential to extend the lifetime of short-lived charges, enhance stability, and improve the performance of interfacial oxidation reactions. Such strategies are vital in achieving efficient and durable photoelectrodes for various energy conversion applications, including solar-driven fuel synthesis.¹⁷

The successful deposition of Ni/CoZnO catalysts on the photoanode led to an impressive photocurrent density at 1.23 V_RHE of 3.50 mA cm⁻². This photocurrent density signifies the ability of the photoanode to generate a substantial flow of electrical current when illuminated with light, indicating efficient charge separation and collection. Furthermore, achieving 99% efficiency is an important accomplishment. The faradaic efficiency refers to the percentage of charge carriers involved in the desired electrochemical reaction compared to the total number of charge carriers generated. In this case, the efficiency suggests that all the generated charge carriers were effectively utilized for the desired oxidation reaction, without any significant loss due to the competing side reactions or charge recombination processes. The ability of the spin-coated film overlayer to simultaneously drive oxidation and proton reduction reactions highlights its multifunctionality and potential as an effective component in photoelectrocatalytic systems. By serving as a catalyst or facilitating charge transfer processes, the spin-coated film overlayer contributes to the overall efficiency and performance of the photoelectrochemical system. These results provide valuable perceptions into the role of photoelectrodes and offer a promising avenue for the development of efficient and sustainable photoelectrocatalytic systems. The ability to drive oxidation reactions and facilitate proton reduction without the need for additional metal or catalyst overlayers simplifies the device architecture and reduces the reliance on costly or scarce materials, the obtained 6.1 mA cm⁻² photocurrent thereby enhancing the feasibility and scalability of the technology.

Results and discussion

In the research study, the absorption spectra and structures of dithiophene-4,8-dione and dimalononitrile are illustrated in Fig. 1, respectively. Dithiophene-4,8-dione, which is a polymer donor, was selected for its use in research due to its wide application in high-performance photovoltaic devices. It has been extensively utilized in blended bulk heterojunctions (BHJs). However, dimalononitrile serves as a non-fullerene acceptor (NFA) in the BHJ system.^18,19 The purpose of this investigation was to examine the role of the dithiophene-4,8-dione overlayer, specifically in the production of long-lived holes in the overall semiconductors. To study this phenomenon, two types of measurements were employed: ultrafast transient absorption and very slow photoinduced absorption. The ultrafast TA measurements allowed them to investigate the dynamics of hole polaron formation and decay on a picosecond timescale. This technique provides insights into the initial stages of charge carrier generation and their subsequent behavior. However, the slow PIA measurements were used to study the long-term behavior of hole polarons, spanning timescales of seconds. By analyzing the PIA signals, it is possible to observe the persistence and stability. Importantly, these investigations were conducted without the addition of any metal oxide or composite material catalyst layer, highlighting the better intrinsic behavior of the dithiophene-4,8-dione/dimalononitrile photoanode and the role of the dithiophene-4,8-dione overlayer in facilitating the generation and persistence of long-lived hole polarons.

Fig. 1 Absorption coefficients of specific materials: dithiophene-4,8-dione and dimalononitrile.

The generation of charges may be in dry solid state, which was investigated using femtosecond transient absorption. A wavelength of 364 nm was used to selectively stimulate the dithiophene-4,8-dione component. The TA spectra of the neat dithiophene-4,8-dione film revealed a broad absorption band corresponding to the singlet exciton of dithiophene-4,8-dione in the near-infrared region, through a peak at 1150 nm, as shown in Fig. 2a. In the spectra of the dithiophene-4,8-dione/dimalononitrile film (Fig. 2c), the amplitude of the dithiophene-4,8-dione exciton absorption at 1150 nm was observed to be reduced, and it decayed more rapidly compared to the neat dithiophene-4,8-dione film (Fig. 3a). This behavior is attributed to ultrafast electron/energy transfer processes occurring in the blended film. These findings are reliable with previous work on bulk heterojunctions and nanoparticles, which have demonstrated similar ultrafast charge transfer dynamics between the donor (dithiophene-4,8-dione) and acceptor (dimalononitrile) components. The reduced amplitude and faster decay of the dithiophene-4,8-dione exciton absorption in the blended film indicate efficient electron transfer from dithiophene-4,8-dione to dimalononitrile, facilitating the separation and generation of charges in the dithiophene-4,8-dione/dimalononitrile photoanodes.²⁰

Fig. 2 Information on time-resolved absorption spectra at various time delays: (a) neat dithiophene-4,8-dione, (b) neat dimalononitrile, (c) dithiophene-4,8-dione and dimalononitrile in the near-infrared probe region (365 nm), and (d) dithiophene-4,8-dione/dimalononitrile in the near-infrared region (750 nm).

Fig. 3 (a) TA kinetics of dithiophene-4,8-dione/dimalononitrile and neat dithiophene-4,8-dione (1140–1150 nm). (b) Normalized kinetics of dithiophene-4,8-dione/dimalononitrile, dithiophene-4,8-dione, and dimalononitrile (980–1000 nm).

In the aforementioned observations, steady-state photoluminescence (PL) measurements were conducted to further support the conclusion of efficient charge transfer in the dithiophene-4,8-dione/dimalononitrile bulk heterojunction (BHJ) photoanode. The PL measurements were performed with excitation at 532 nm. The results of the PL measurements demonstrated strong quenching of both dithiophene-4,8-dione and dimalononitrile photoanode excitons in the BHJ structure (Fig. S1, ESI†). This quenching indicates effective charge separation and transfer between the dithiophene-4,8-dione/dimalononitrile components, leading to the generation of free charges. Importantly, the presence of the dithiophene-4,8-dione overlayer did not significantly alter the decay kinetics of the film (as evident from the decay kinetics of the dithiophene-4,8-dione/dimalononitrile film shown in Fig. 3a). This suggests that the dithiophene-4,8-dione overlayer does not interfere with the ultrafast electron/energy transfer process in the BHJ structure. The similar decay kinetics observed in the film further supports the dithiophene-4,8-dione overlayer, which may not affect the efficient charge transfer and generation of charges within the BHJ system. The dithiophene-4,8-dione exhibits hole transfer kinetics that are typical of NFA:polymer blends. Hole transfer kinetics were investigated by femtosecond TA spectroscopy with a pump wavelength of 750 nm. This choice of excitation wavelength is based on the absorption spectra of dithiophene-4,8-dione and dimalononitrile, as shown in Fig. 1. The results of this observation provide insights into the electronic properties and behavior of the dithiophene-4,8-dione film at 750 nm, indicating that it may have a different response compared to other states or electronic transitions within the material. To gain a more comprehensive understanding, it would be necessary conduct TA measurements and their interpretation. The TA spectra of the dithiophene-4,8-dione/dimalononitrile film revealed that GSB obtained signals within the absorption region 550–650 nm. This observation indicates the ultrafast migration of ions from dimalononitrile to dithiophene-4,8-dione upon photoexcitation of dimalononitrile. The signals obtained by GSB originated from dithiophene-4,8-dione in the absorption region, which confirms the efficient transfer of holes from dimalononitrile to dithiophene-4,8-dione within the dithiophene-4,8-dione/dimalononitrile photoanodes. The ultrafast nature of this hole transfer is supported by the observed GSB signals in the TA spectra. The similarity in the hole transfer kinetics between dithiophene-4,8-dione and dimalononitrile photoanodes further highlights the role of the dithiophene-4,8-dione overlayer, as the presence of the overlayer does not significantly affect the hole transfer process. This supports the conclusion that the dithiophene-4,8-dione overlayer does not interfere with the ultrafast electron/energy transfer from dithiophene-4,8-dione to dimalononitrile and the subsequent hole transfer from dimalononitrile to dithiophene-4,8-dione in the BHJ system. When the near-infrared (NIR) region is probed at an excitation wavelength of 750 nm, the TA spectra of the dimalononitrile reveal the absorption of singlet exciton of dimalononitrile through a peak at 930 nm (Fig. 2b). The absorption peak observed in the NIR region for the dithiophene-4,8-dione and dimalononitrile films is broader, with shoulders at approximately 1000 nm. By probing the film at 980–1000 nm with different pump fluences, the corresponding kinetics of the photogenerated polarons was examined. The results indicate the kinetics of the heterojunction film. This kinetics is attributed to the rejoining of photogenerated polarons within the dithiophene-4,8-dione and dimalononitrile films. Notably, the polaron feature exhibits stable and long-time decay of over 6 nanoseconds (ns) under low excitation fluence. The photoinduced absorption kinetics decay of the dimalononitrile film may be complete in approximately 100 picoseconds (ps) (Fig. 3b). The significant difference in the decay kinetics suggests that the presence of the dithiophene-4,8-dione overlayer and the formation of the dithiophene-4,8-dione/dimalononitrile heterojunction contribute to the stabilization and the prolonged time of the photogenerated polarons. Under low excitation fluence, the polarons generated in the dithiophene-4,8-dione/dimalononitrile film exhibit long-time decay, indicative of enhanced charge separation and suppressed recombination processes compared to the neat dimalononitrile film. The comparison between the dithiophene-4,8-dione/dimalononitrile photoanode and the film without the dithiophene-4,8-dione overlayer revealed significant differences in the full recombination kinetics and the production of long-lived polarons (Fig. 3b). The dithiophene-4,8-dione/dimalononitrile photoanode exhibited nearly threefold slower rejoining kinetics. This suggests that the presence of the dithiophene-4,8-dione overlayer assists in the three-dimensional charge separation, even on the timescale of picoseconds. The retardation of charge rejoining in the dithiophene-4,8-dione/dimalononitrile photoanode is a notable advantage, as it contributes polarons that remain long-lived (as given Fig. S2†). The enhanced spatial separation of charges and the suppression of bimolecular recombination facilitated by the dithiophene-4,8-dione overlayer are crucial factors in driving photocatalytic reactions. By retarding charge recombination, the dithiophene-4,8-dione/dimalononitrile photoanode promotes the extended lifetime of polarons, which enhances the chances for charge carriers to participate in desired photocatalytic reactions.

This contributes to more stable and long-lived polarons and retards bimolecular charge recombination, making the photoanode more suitable for driving efficient photocatalytic reactions. This rapid transfer results in the separation of dimalononitrile excitons, indicating fast exciton dissociation in dithiophene-4,8-dione/dimalononitrile. Additionally, hole transfer from dimalononitrile to dithiophene-4,8-dione takes place within approximately 2 ps, indicating the rapid transfer of holes between the two components. This further supports the efficient charge separation in the dithiophene-4,8-dione/dimalononitrile system. The right panel of the figure illustrates that introducing the dithiophene-4,8-dione overlayer on the bulk heterojunction photoanode causes a three times increase in the longtime of polarons. This indicates that the dithiophene-4,8-dione overlayer contributes to the extended lifetime of polarons, highlighting its role in promoting charge separation and reducing charge recombination. Furthermore, the neat dithiophene-4,8-dione film exhibits a very partially red-shifted absorption compared to the dithiophene-4,8-dione/dimalononitrile film. This difference suggests very stronger aggregation in the neat dithiophene-4,8-dione film compared to the film (as shown in S3†). Overall, the findings demonstrate the effective quenching of dithiophene-4,8-dione excitons through ultrafast electron and energy transfer processes in the dithiophene-4,8-dione/dimalononitrile system. The slight shift in ground-state absorption between the neat dithiophene-4,8-dione film and the blend film suggests molecular aggregation differences and potential energetic variations within the blend system.²¹

The spatial charge separation of holes achieved through the incorporation of a spin-coated film overlayer, such as dithiophene-4,8-dione, contributes to the retardation of bimolecular recombination compared to the dithiophene-4,8-dione/dimalononitrile BHJ alone. This enhanced charge separation, aided by the spin-coated film overlayer, can be expected to improve the functionality of the photoanode for photoelectrochemical systems. The presence of the dithiophene-4,8-dione overlayer on the dithiophene-4,8-dione/dimalononitrile photoanode creates a favorable environment for hole extraction and reduces the likelihood of charge recombination events. The consideration of energy level alignment and further development of spin-coated film overlayers are crucial for advancing the cell technology of photoelectrochemistry. To investigate the charge kinetics in the presence of electrolytes and under operando photoelectrochemical (PEC) conditions, the photoanodes were studied by photoinduced absorption (PIA) spectroscopy. This technique allowed for the examination of charge dynamics on longer timescales.²² Under PEC conditions, the PIA kinetics were measured using pulsed LED excitation with a duration of 5 seconds. The measurements were conducted in the presence or absence of hydrogen peroxide and with an applied bias of 1.23 V_RHE. A three-electrode configuration was employed; the experiments were carried out in 1 M phosphate buffer solution (pH 8.5). To collect the PIA kinetics on the second timescales, the differences in absorbance at different wavelengths were measured. The electrochemical measurement of the cell fully exposed the pulses of LED (light-emitting diode), with a greater power density of 39.5 mW cm⁻² at 356 nm. The LED pulses were applied for 5 seconds with a subsequent 5 second off period, and this cycle was repeated (as shown in S4†). The measurements were performed through the glass/indium tin oxide interface, allowing the probe light to illuminate the sample and the resulting PIA signals to be recorded. This experimental setup enabled the investigation of charge dynamics and the impact of electrolytes, such as hydrogen peroxide, on the photoanodes under conditions of photoelectrochemical reactions. By monitoring the PIA kinetics on longer timescales, a deeper understanding of the charge transport and recombination processes in the presence of electrolytes could be obtained. In the absence of an applied external bias to the photoelectrochemical (PEC) cells, the recorded photoinduced absorption (PIA) signals from the dithiophene-4,8-dione/dimalononitrile photoanodes are negligible, measuring less than 0.25 milli-optical density (mOD). This observation holds true regardless of the presence of hydrogen peroxide. The fast bimolecular recombination process in the dithiophene-4,8-dione/dimalononitrile system has been demonstrated to be more relevant for the ultrafast transient absorption results obtained using higher intensity pulses of laser.¹⁸ The mentioned study showed that, under 1 sun illumination, dithiophene-4,8-dione/dimalononitrile solar cells exhibit fast bimolecular recombination occurring on the microsecond timescale. This supports the notion that charge recombination in the dithiophene-4,8-dione/dimalononitrile system is a fast process, further emphasizing the need for efficient charge separation and suppression of recombination mechanisms to enhance the performance of these devices. Overall, the negligible PIA signals obtained in the absence of external bias in the dithiophene-4,8-dione/dimalononitrile photoanodes indicate the occurrence of rapid charge recombination processes on the nanosecond timescale, consistent with the previous findings of fast bimolecular recombination in dithiophene-4,8-dione/dimalononitrile solar cells even under 1 sun illumination. Remarkably, dithiophene-4,8-dione/dimalononitrile photoanodes exhibited long-lived PIA signals on the second timescale (950 nm) scavenger such as hydrogen peroxide (Fig. 4c). These signals can be attributed to the presence of stable and long-lived dithiophene-4,8-dione⁺ polarons, as reported previously.¹⁶ This indicates that the presence of dithiophene-4,8-dione in a better way increases the buildup of photogenerated charges that remain long-lived. These findings are consistent with the fast transient absorption, as given in Fig. 2. Furthermore, the signals of PIA kinetics of photoanodes below the bias, except the presence of hydrogen peroxide, were probed across a wavelength range of 600 to 1000 nm. The dithiophene-4,8-dione overlayer in the dithiophene-4,8-dione/dimalononitrile photoanode render the charges stable and long-lived, as indicated by the longer and more amplitude of the dithiophene-4,8-dione polaron features. The PIA kinetics across the measured wavelength range provides further insights into the charge dynamics and behavior of the photoanodes under bias in the absence of hydrogen peroxide. Indeed, the long-lived charge accumulation observed in the dithiophene-4,8-dione/dimalononitrile photoanode, as well as its enhancement by the dithiophene-4,8-dione overlayer, highlight the functional significance of this layer. The mechanical origin of such long lifetime carriers in photoelectrodes based on the organic polymer has not yet been properly established although it is clearly enhanced by the dithiophene-4,8-dione overlayer, highlighting the functional importance of this layer in materials. In non-precious metal oxide systems, this phenomenon is often attributed to the formation of a space charge layer at the semiconductor/electrolyte interface.

Fig. 4 Photoinduced absorption of dithiophene-4,8-dione/dimalononitrile: (a) in 1 M phosphate buffer and (b) 0.2 M of hydrogen peroxide in a 1 M phosphate buffer solution at 1.23 V_RHE. PIA kinetics of the dithiophene-4,8-dione/dimalononitrile: (c) without and (d) with 0.2 M hydrogen peroxide.

However, in the case of photoelectrodes, the origin of such long-lived charge accumulation is not yet fully established and the specific mechanisms behind this extended charge accumulation in systems are still under investigation. However, the presence of the dithiophene-4,8-dione overlayer clearly enhances this phenomenon. The dithiophene-4,8-dione overlayer probably plays a role in improving charge separation, minimizing charge recombination, and facilitating the growth of polarons, and the stable charges remain for a long time in the photoanode. The precise mechanisms underlying these effects require further study and characterization. Nonetheless, the observed functional importance of the dithiophene-4,8-dione overlayer in enhancing the long carrier lifetime underscores its significance in achieving efficient charge accumulation and improved performance in photoelectrodes. Continued research in the field to gain an understanding of the mechanisms driving these phenomena will aid in the further development and optimization of photoelectrode systems. When 0.2 M hydrogen peroxide is incorporated into 1 M phosphate buffer, insignificant photoinduced absorption signals were detected for dithiophene-4,8-dione/dimalononitrile photoanodes (Fig. 4d). This observation indicates that the long-lived dithiophene-4,8-dione polarons are present on the photoanodes for hydrogen peroxide, in the presence of electrolytes. Similarly, scavenger holes, used in 1 M phosphate buffer, and PIA signals with lower amplitudes were detected. The efficient quenching of the long-lived polarons by the sacrificial hole scavengers demonstrates their role in facilitating charge extraction and preventing recombination processes. By providing an alternative pathway for the extracted holes, the sacrificial hole scavengers help maintain the charge balance and minimize charge recombination in the photoanodes. These findings highlight the importance of proper charge management and the role of sacrificial hole scavengers in enhancing the performance of photoelectrodes. The efficient quenching of the long-lived polarons by hydrogen peroxide in the electrolyte provides valuable insights for optimizing the operation of photoanodes and achieving enhanced photoelectrochemical functionality. The photoelectrochemical performance of the dithiophene-4,8-dione/dimalononitrile photoanodes was evaluated using a three-electrode configuration in the presence of electrolytes consisting of 0.2 M hydrogen peroxide in 1 M phosphate buffer, as shown in a Fig. 5. LSV scan rates of the dithiophene-4,8-dione/dimalononitrile photoanodes were conducted under chopped condition at a bias of 1.23 V_RHE, however, the second dithiophene-4,8-dione/dimalononitrile photoanode exhibited a slightly lower photocurrent of 5.0 mA cm⁻² density. Although this value is lower than that of the first photoanode, it still indicates a reasonable photocurrent density, albeit slightly less efficient in comparison. The J_ph value obtained by the dithiophene-4,8-dione/dimalononitrile photoanode is max 6.1 mA cm⁻², which can resourcefully catalyze the reactions completely, in particular the oxidation of hydrogen peroxide, except the need for metal oxides or composite catalysts. This result highlights the potential of photoanodes as efficient catalysts for photoelectrochemical reactions. The incorporation of the dithiophene-4,8-dione overlayer on the dithiophene-4,8-dione/dimalononitrile photoanode contributes to the enhanced photoelectrochemical performance, as evidenced by the higher photocurrent density achieved (Fig. 6).

Fig. 5 EQE of the dithiophene-4,8-dione/dimalononitrile absorption spectrum and photoanode and dithiophene-4,8-dione/dimalononitrile.

Fig. 6 Theoretical hydrogen evolution yield from the Pt counter electrode at 1.23 V_RHE in 0.2 M buffer under continuous 1 sun illumination, and the corresponding faradaic efficiency. The accumulated hydrogen yield is measured by the Clark electrode (unisense).

These findings reveal the possibilities of utilizing materials as active components in photoelectrochemical devices, offering a sustainable and efficient approach for the catalysis of chemical reactions using light energy. The improved performance of the photoanode, facilitated by the presence of long-lived polarons induced by the dithiophene-4,8-dione overlayer, is clearly demonstrated. This enhancement is not only reflected in the increased photocurrent density but also in the coupled hydrogen evolution observed in the photoelectrochemical (PEC) cell operation. The photograph of the cell of photoelectrochemical process showcases the successful coupling of hydrogen evolution with the photoanode performance. This indicates the effective utilization of the photo-generated charges for driving the desired hydrogen evolution reaction. Additionally, the efficiency for the coupled hydrogen evolution of the dithiophene-4,8-dione/dimalononitrile photoanode at 1.23 V_RHE in 0.2 M hydrogen peroxide in 1 M phosphate buffer under continuous illumination of 1 sun is approximately 74%. This indicates that three-quarters of the photocurrent generated by the photoanode was utilized for the desired hydrogen evolution reaction. However, approximately a quarter of the photocurrent was involved in undesired reactions within the photoelectrochemical device. Further development and efforts can focus on understanding and mitigating these undesired reactions affecting the overall performance of photoelectrochemical devices. Overall, the presence of the dithiophene-4,8-dione overlayer enhances the photoanode performance, leading to efficient coupled hydrogen evolution. However, careful evaluation and optimization of the faradaic efficiency is necessary to maximize the desired reaction and minimize side reactions in order to achieve higher overall photoelectrochemical efficiency. The dithiophene-4,8-dione/dimalononitrile photoanode showed a higher J_ph than the dithiophene-4,8-dione photoanode, indicating that the extended carrier lifetime of the dimalononitrile overlayer improves the oxidative performance of the photoanode with various hole sacrificial agents and improves the carrier lifetimes. The noteworthy J_ph value of 6.1 mA cm⁻² clearly demonstrates that film layer photoanodes are based directly on light absorbers. It obviously proves that the long-lived charges of the dimalononitrile overlayer further improve the photoanode performance. The J_ph signal response from the film photoanode creates direct light which fully absorbs and fully catalyzes electrochemical reactions, except those involving metal oxides. This demonstrates that the dithiophene-4,8-dione layer advances the photoanode response and hydrogen evolution. The faradaic efficiency of the H₂ evolution reaction of the dithiophene-4,8-dione/dimalononitrile photoanode at 1.23 V_RHE in 0.2 m buffer under 1 sun illumination shows that a quarter of the photocurrent is used for unsought reactions in this PEC device. The measured & theoretical amount of H₂ from the Pt counter electrode at 1.23 V_RHE in buffer under continuous 1 sun illumination and the corresponding faradaic efficiency are reported. Accumulated H₂ amounts are measured by the Clark electrode. Theoretical hydrogen amounts were determined by dividing the measured photogenerated charges by 2F. A constant value of 96 500 C mol⁻¹ is reported in Fig. 5 and the dithiophene-4,8-dione/dimalononitrile photoanode is shown to exhibit a higher photocurrent density (J_ph). The higher photocurrent in the case of hydrogen peroxide oxidation is attributed to the higher oxidation potential of hydrogen peroxide (approximately −4.7 eV).¹⁶ This indicates that the highest occupied molecular orbital (HOMO) of dithiophene-4,8-dione (round off −5.4 eV) possesses an appropriate potential for oxidizing hydrogen peroxide. The results indicate the favorable energy level alignment between the dithiophene-4,8-dione overlayer and the sacrificial hole agents, which contributes to efficient charge transfer and oxidation reactions in the photoanode. The extended carrier lifetime provided by the dithiophene-4,8-dione overlayer enhances the overall oxidation performance of the photoanode, enabling higher photocurrents even when utilizing different sacrificial hole agents. The dependence of the dithiophene-4,8-dione/dimalononitrile photoanode performance on the thickness of the dithiophene-4,8-dione overlayer was investigated by varying the concentration of the dithiophene-4,8-dione solution, resulting in different thicknesses of the overlayer. LSV measurements were performed to evaluate the performance of the photoanode with different dithiophene-4,8-dione overlayer thicknesses (30, and 45 nm, achieved by concentrations of 15, and 20 mg mL⁻¹, respectively). Further, the dependence of the dithiophene-4,8-dione/dimalononitrile photoanode performance on the thickness of the dimalononitrile overlayer was investigated by controlling the concentration of dimalononitrile solution, as seen in Fig. 7 (15, 30, & 45 nm). The dimalononitrile film showed high uniformity over the substrates. This suggests that within this range, the thickness variation of the dithiophene-4,8-dione overlayer does not significantly impact the photoanode performance.

Fig. 7 LSV scans of the dithiophene-4,8-dione/dimalononitrile photoanodes with different thicknesses of overlayer in 0.2 M hydrogen peroxide in 1 M phosphate buffer under 1 sun illumination.

However, when the thickness of the dithiophene-4,8-dione overlayer was further increased to 45 nm, the photocurrent drastically decreased to approximately 1.5 mA cm⁻². This decrease in photocurrent indicates the limited conductivity in the dithiophene-4,8-dione film at this thickness, which negatively affects the charge transport and overall performance of the photoanode. The decrease in photocurrent with a thicker dithiophene-4,8-dione overlayer highlights the importance of achieving an optimal balance between the thickness of the dithiophene-4,8-dione overlayer and its conductivity for efficient charge transport and photoelectrochemical performance. The choice of an appropriate thickness is crucial to maintain good charge transport properties within the photoanode. The careful optimization of the dithiophene-4,8-dione overlayer thickness to ensure both efficient charge separation and effective charge transport ultimately leads to enhanced photoelectrochemical performance in the dithiophene-4,8-dione/dimalononitrile photoanode. Indeed, the highest photocurrent density (J_ph) is 6.1 mA cm⁻². The dithiophene-4,8-dione overlayer thickness is 30 nm, as observed in the study. Interestingly, the onset potential, which corresponds to the applied bias required to initiate the transfer of photogenerated charges from the bulk heterojunction (BHJ) to the surface of the dithiophene-4,8-dione overlayer was reduced from 0.4 to 0.2 V_RHE when the dithiophene-4,8-dione thickness was decreased from 45 to 15 nm. This reduction in onset potential with the decrease in dithiophene-4,8-dione thickness is consistent with the observations from Fig. 5, where the dithiophene-4,8-dione overlayer on the dithiophene-4,8-dione/dimalononitrile photoanode led to a lower onset potential than that the dithiophene-4,8-dione/dimalononitrile photoanode without the overlayer. The results suggest that a greater applied bias is required when using a very thicker dithiophene-4,8-dione overlayer to efficiently transfer photogenerated charges from the BHJ onto their surface area. This indicates that carrier diffusion within the semiconductors, such as dithiophene-4,8-dione, can become limiting for the thicknesses. Therefore, it is crucial to optimize the spin-coated film's thickness to ensure that the diffusion career restrictions of the material semiconductors are not exceeded. Finding the right balance between the dithiophene-4,8-dione overlayer thickness and the applied bias can help maximize the charge transfer efficiency and overall performance of the photoanode. These findings highlight the importance of careful thickness optimization of the spin-coated film overlayer to achieve efficient charge transfer and to prevent limitations imposed by semiconductors through carrier diffusion. For dithiophene-4,8-dione, the EQE value provides insights into the device's ability to harvest light and convert it into electrical current or produce light emission. Higher EQE values indicate higher conversion efficiency, meaning that a larger fraction of incident photons are converted into useable electrical charges. Improving the EQE of optoelectronic devices is crucial for enhancing their overall performance and energy conversion efficiency. Researchers and engineers focus on optimizing materials, device structures, and fabrication techniques to maximize the EQE in various applications. In this case, the EQE spectrum of the photoanode was determined under the specified conditions of having 0.2 M concentration of hydrogen peroxide (H₂O₂) and 1 M phosphate buffer at pH 5.5. These conditions were likely chosen to investigate the photoanode's performance and efficiency in a specific environment or electrochemical setup at a bias of 1.23 V_RHE. These conditions were likely chosen to investigate the photoanode's performance and efficiency in a specific environment or electrochemical setup. The EQE spectrum shows photo-responses across the wavelength range of approximately 900 nm, which corresponds to dithiophene-4,8-dione/dimalononitrile. This high EQE value suggests that the device has a strong capability to absorb and convert photons from the 850 nm light source. It could be an indication of optimized material properties, efficient carrier generation, reduced recombination losses, or improved charge collection mechanisms within the device, and the photoanodes are responsible for absorbing photons and initiating the conversion of light energy into electrical current. The dithiophene-4,8-dione/dimalononitrile photoanode demonstrated efficient absorption and utilization of photons at 900 nm, which aligns with the absorption of dimalononitrile. However, the EQE of dithiophene-4,8-dione for the absorption is comparable to the EQE observed in the dimalononitrile absorption region (700–900 nm). These obtained results specify that while the dithiophene-4,8-dione overlayer influences the maximum absorption wavelength range towards its own absorption properties, the dimalononitrile molecules still play a dominant role in the overall photon-to-current conversion process. The dimalononitrile molecules contribute to the majority of the EQE and are primarily responsible for the efficient conversion of photons into photocurrent in this photoanode configuration. The EQE measurements provide valuable insights into the spectral response and light absorption characteristics of the dithiophene-4,8-dione/dimalononitrile photoanode, highlighting the contribution of both dimalononitrile and dithiophene-4,8-dione components to the overall photocurrent generation. Based on the information provided, it seems that the primary function of the dithiophene-4,8-dione overlayer is not to act as a light sensitizer, but rather as an interlayer positioned between the dithiophene-4,8-dione/dimalononitrile nanoparticles and the electrolyte. This interlayer serves to enhance carrier lifetimes within the photoelectrode configuration.

The maximum external quantum efficiency (EQE) of dithiophene-4,8-dione/dimalononitrile nanoparticles, when combined with a 10% Pt catalyst, was 5.0% in a 0.2 M ammonium acetate solution. However, the configuration of a photoelectrode incorporating overlayers of films shows better efficiencies than the photoelectrode under an applied bias. This suggests that the presence of the dithiophene-4,8-dione layers strongly affect the performance of the photoelectrode system by enhancing its efficiency beyond what the nanoparticles alone can achieve. Overall, it appears that the dithiophene-4,8-dione overlayer acts as an effective interlayer in the photoelectrode configuration, enhancing the carrier lifetime and leading to higher efficiencies when compared to the photocatalytic nanoparticles alone. According to the provided information, chronoamperometry measurements were conducted to evaluate the operational stability of the system. These measurements were performed in 0.2 M hydrogen peroxide in 1 M phosphate buffer under 1 sun illumination at an applied potential of 1.23 V_RHE, as shown in Fig. 8. It was observed that when the dithiophene-4,8-dione overlayer was present in the system, the photocurrent was stable at 39% at 2500 seconds, even without the presence of an encapsulation layer. In contrast, in the absence of the dithiophene-4,8-dione overlayer, the photocurrent decayed to less than 19% of the initial value within 1000 seconds. The finding suggests that the dithiophene-4,8-dione overlayer plays a crucial role in improving the underwater stability of the system. The hydrophobic nature of the dithiophene-4,8-dione overlayer is likely responsible for this enhanced stability. The presence of the dithiophene-4,8-dione overlayer enhances the operational stability of the system by stabilizing the photocurrent over an extended period, even without the use of an encapsulation layer. The hydrophobic nature of the dithiophene-4,8-dione overlayer is believed to contribute to this improved stability. Based on the obtained information, in the dithiophene-4,8-dione/dimalononitrile photoanodes, stable and long-lived signals are only detected at the Pt counter electrode. The electrical driving force is necessary, which may be responsible for the growth of polarons on the surface of electrode, where the reaction of photocatalytic takes place. The hydrophobic nature of the organic thin film used in this system limits their contact with water (electrolyte), resulting in the electrolyte interface primarily occurring at the surface of the film area. The bias-dependent photocurrent generation shown in Fig. 5 suggests that electrical forces are required to facilitate the accumulation of polarons at the electrode surface and remain durable and stable. It is hypothesized that the dithiophene-4,8-dione/dimalononitrile nanoparticle suspensions may allow for greater water dispersion, facilitating the generation of charges for the semiconductor. Additionally, the hydrophilicity of the surface area could be explored as a means to further investigate and optimize the system's performance. The hydrophobic nature of the thin film limits their interaction with the electrolyte, necessitating an electrical driving force for efficient photocurrent generation. The information provided highlights the challenges and advantages of buried bulk heterojunctions (BHJ) in combination with photoanodes for water splitting catalysis. Buried bulk heterojunction photoanodes are an amalgamation of photovoltaics (PV) and water splitting catalysis. It is highly necessary to protect the component from direct contact with water (electrolyte) through photovoltaics. Additionally, a metal oxide interlayer is needed to transfer charges through photogeneration to fully initiate the catalytic reaction mechanism. Such systems may have very limited cost advantage over separated photovoltaic-electrolyser cells in terms of hydrogen generation cost.²³ Alternatively, carbon-based nitride photoanodes were reported with relatively low photocurrent, maximum at round of 0.1 mA cm⁻². In contrast, the described dithiophene-4,8-dione/dimalononitrile photoanode achieves higher photocurrent. It appears that the mentioned experiment achieved a higher photocurrent of 6.1 mA cm⁻² and an external quantum efficiency (EQE) of 17.3%, while conducting the hydrogen evolution reaction (HER) utilizing a direct electrolyte. These results indicate promising progress in the field of photo electrochemistry, where simultaneous photocurrent generation and hydrogen evolution are achieved with high efficiency. This is made possible by the presence of the dithiophene-4,8-dione overlayer, which generates long-lived charges. However, it should be noted that the high photocurrent and EQE in the dithiophene-4,8-dione/dimalononitrile photoanode are determined using an electric bias and the oxidation of hydrogen peroxide. The contests still endure in controlling the composite materials' hydrophilicity and best energetics characteristic of the composite spin-coated film to fully reduce the potential and fully support water splitting and oxidation processes at a high level. Finally, BHJ photoanodes offer an amalgamation of water oxidation and OPV catalysis, but their cost advantage over separate photovoltaic-electrolyzer cells is limited. The dithiophene-4,8-dione/dimalononitrile photoanode shows promising results with high photocurrent and EQE values.

Fig. 8 Chronoamperometry curves under 1 sun illumination in 0.2 M hydrogen peroxide in a 1 M phosphate buffer solution at 1.23 V_RHE. The chronoamperometry measurements were carried out without stirring.

Conclusion

Further studies are warranted to elucidate the specific mechanisms by which a spin-coated film overlayer drives oxidation reactions and facilitates charge transfer processes. Understanding these mechanisms will enable the optimization of the spin-coated film overlayer design and its integration into advanced photoelectrochemical systems for various energy conversion applications. The oxidation photocurrent of 6.1 mA cm⁻², tied with H₂ gas generation, is achieved in the absence of metal or metal oxide electrocatalysts. This suggests that the spin-coated film overlayer, in combination with the photoanode, exhibits efficient charge separation, promotes the desired oxidation reactions without the need for additional catalytic materials and plays a critical role of the film overlayer in enhancing polaron kinetics, extending the charge lifetime and driving efficient photo electrocatalytic performance. The ability to achieve high photocurrents and H₂ generation without metal or metal oxide electrocatalysts underscores the potential of the photoanode with the film overlayer as a promising platform for sustainable energy conversion applications. Further investigations are required to gain a deeper understanding of the mechanisms underlying the extended charge lifetime and improved photoelectrocatalytic performance facilitated by the spin-coated film overlayer. This knowledge will contribute to the continued advancement and optimization of photoanodes for efficient and scalable solar-driven fuel synthesis.

Data availability

The authors declare that the data supporting the findings of this study are available upon request.

Author contributions

Abdul Qayoom Mugheri, supervision, investigation, conceptualization, writing – original draft writing and review & editing final version. Muhammad Youns Laghari and Kashif Ali, resources. Ali Asghar Sangha and Kashif Ali, formal analysis. Kashif Ali, Nadeem Ahmed Mugheri, Muhammad Rajib Soomro, Muhammad Ishfaq Chohan and Arsalan Ahmed Mugheri, data curation, software and validation, technical visualization Aftab Kandhro & Mazhar Iqbal khaskheli.

Conflicts of interest

There are no conflicts to declare.

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Footnote

† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ra05126a

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