Advanced TiO₂-Based Photoelectrocatalysis: Material Modifications, Charge Dynamics, and Environmental–Energy Applications

Abstract

This review presents a comprehensive overview of recent advances in TiO₂-based photoelectrocatalysis (PEC), with an emphasis on material design strategies to enhance visible-light responsiveness and charge carrier dynamics. Key approaches—including elemental doping, defect engineering, heterojunction construction, and plasmonic enhancement—are systematically discussed in relation to their roles in modulating energy band structures and promoting charge separation. Beyond fundamental mechanisms, the review highlights the broad environmental and energy-related applications of TiO₂-driven PEC systems, encompassing the degradation of persistent organic pollutants, microbial disinfection, heavy metal removal, photoelectrochemical water splitting for hydrogen production, and CO₂ reduction. Recent progress in integrating PEC systems with energy harvesting modules to construct self-powered platforms is critically examined. Current limitations and future directions are also outlined to guide the rational development of next-generation TiO₂-based photoelectrocatalytic systems for sustainable environmental remediation and solar fuel conversion.

1. Introduction

Water pollution arising from organic contaminants released via agricultural runoff, industrial effluents, and diverse anthropogenic activities has become a pressing global environmental concern over recent decades. Many of these pollutants are classified as emerging contaminants, notable for their persistence in aquatic environments and resistance to degradation by conventional wastewater treatment processes. Such recalcitrant substances—including synthetic chemicals, industrial dyes, pharmaceutical residues, and agrochemicals like pesticides—pose significant ecological and public health risks due to their established toxicity, mutagenicity, and carcinogenic potential [1,2,3,4,5]. Notably, approximately 300,000 tons of dye-contaminated effluents from textile industries are annually discharged into water bodies worldwide, significantly deteriorating water quality and adversely impacting aquatic biodiversity [5,6].

Conventional wastewater treatments, comprising biological, physicochemical, and chemical methods, have demonstrated limited efficacy in eliminating persistent organic pollutants (POPs), primarily due to these compounds’ inherent chemical stability and low biodegradability [7,8,9,10,11,12,13]. In addressing this challenge, advanced oxidation processes (AOPs) have emerged as a promising alternative, utilizing highly reactive species to effectively degrade recalcitrant contaminants [14,15,16]. Among various AOPs, photoelectrocatalysis (PEC) has attracted considerable scientific attention due to its superior efficiency compared to traditional photocatalysis. PEC synergistically combines photocatalytic and electrochemical oxidation mechanisms, overcoming limitations inherent in the standalone applications of each method [17,18,19]. This growing interest in PEC is reflected in the sharp increase in scientific publications over the past two decades, as illustrated in Figure 1.

In PEC, an external bias voltage is applied across a semiconductor-based photocatalyst immobilized on a conductive substrate. Illumination with photons of energy equal to or greater than the semiconductor’s bandgap results in the excitation of electrons from the valence to the conduction band, generating electron–hole pairs. The external bias promotes rapid separation of these charge carriers, directing electrons toward the cathode and holes toward the photoanode interface, thus effectively mitigating recombination—a significant limitation of conventional photocatalysis—and enhancing quantum efficiency and degradation performance [20,21,22].

Among the semiconductor materials explored, titanium dioxide (TiO₂) stands out as the most extensively investigated due to its exceptional intrinsic photocatalytic activity, chemical and thermal stability, environmental friendliness, resistance to photocorrosion, and cost-effectiveness [23,24,25]. Since Fujishima and Honda first demonstrated TiO₂-based photoelectrochemical water splitting in 1972 [21], TiO₂ has been extensively studied for diverse environmental applications, including water and air purification and solar energy conversion.

Nevertheless, pristine TiO₂ exhibits critical limitations hindering practical application, notably its wide bandgap (3.0–3.2 eV), restricting optical absorption primarily to the ultraviolet region (~5% of the solar spectrum), and a high recombination rate of photogenerated electron–hole pairs, significantly reducing quantum efficiency [26,27,28]. These intrinsic drawbacks have prompted substantial research into modifying TiO₂ to enhance visible light absorption and improve charge carrier dynamics.

Numerous strategies have emerged to address these limitations, including elemental doping (with metals and non-metals), defect engineering, heterojunction design, and exploitation of surface plasmon resonance (SPR) effects [29,30,31,32]. These approaches aim to modify the electronic structure of TiO₂, narrowing its bandgap, extending absorption to visible wavelengths, and enhancing charge separation and carrier transport. Advances in nanomaterial synthesis and cutting-edge characterization techniques have accelerated the development of advanced TiO₂-based PEC systems with improved visible-light-driven performance [33,34].

The application of TiO₂-based PEC systems in environmental remediation has demonstrated substantial potential, effectively degrading diverse organic pollutants, such as dyes, pharmaceuticals, pesticides, and industrial chemicals [35,36,37]. This process relies predominantly on the in situ generation of highly reactive oxidative species, primarily hydroxyl radicals (•OH), which non-selectively mineralize organic contaminants into innocuous end-products like CO₂ and H₂O. Beyond organic pollutants, PEC also facilitates heavy metal reduction and immobilization, microbial pathogen inactivation, and simultaneous pollutant degradation and energy generation [38,39,40].

Despite these promising advances, several critical barriers remain for large-scale implementation of TiO₂-based PEC technologies, including limited visible light utilization, moderate quantum efficiencies, inadequate long-term operational stability, and challenges associated with scaling laboratory successes into commercially viable systems (Figure 2) [3,41,42]. Addressing these barriers necessitates deeper mechanistic insights into PEC processes at the materials, interfaces, and system levels, and the establishment of robust design principles for catalytic efficacy and durability. A general schematic of the photoelectrochemical (PEC) process using a TiO₂ photoanode is illustrated in Figure 1, highlighting the roles of photogenerated electrons and holes in redox reactions occurring at the photoanode and cathode.

This review critically evaluates recent advances in TiO₂-based PEC technologies, emphasizing strategies for enhanced visible light activation and improved environmental applicability. Initially, we elucidate fundamental physicochemical mechanisms underlying TiO₂ PEC, followed by an in-depth assessment of materials engineering strategies—including doping, defect modulation, heterojunction formation, and plasmonic enhancement—to expand the visible photoresponse and improve charge separation. Subsequently, we examine the environmental applications of advanced PEC systems, particularly organic contaminant degradation, water purification, and energy-related processes. Finally, we identify persistent technical challenges and explore emerging research directions, guiding the rational development of next-generation TiO₂-based PEC platforms for sustainable environmental remediation.

2. TiO₂ Photoelectrocatalysis Mechanisms

2.1. Fundamental Principles of TiO₂ Photoelectrocatalysis

Photoelectrocatalysis (PEC) represents a substantial advancement over conventional photocatalysis by coupling semiconductor-driven photophysical processes with electrochemical charge transfer reactions, effectively addressing the major limitation of rapid recombination of photogenerated electron–hole pairs (Figure 3) [43]. Upon illumination with photons possessing energies equal to or exceeding the bandgap of TiO₂ (approximately 3.2 eV for anatase, 3.0 eV for rutile), electrons in the valence band (VB) are excited to the conduction band (CB), generating electron–hole pairs [44,45]. The application of an external anodic bias at the TiO₂ photoanode creates an internal electric field that directs electrons towards the cathode, thus significantly reducing recombination rates [46,47]. This configuration enhances the oxidative potential of photogenerated holes (located around +2.7 V vs. NHE at neutral pH), facilitating direct oxidation of organic pollutants and formation of reactive oxygen species (ROS), particularly hydroxyl radicals (•OH), leading to pollutant mineralization into CO₂ and H₂O [48,49].

2.2. Charge Separation and Transfer Mechanisms

The efficiency of charge separation and interfacial charge transfer in TiO₂-based PEC systems is governed by factors including the crystalline phase of TiO₂, substrate conductivity, applied external bias, and electrolyte composition [50,51]. Among the polymorphs of TiO₂—anatase, rutile, and brookite—anatase typically exhibits superior PEC performance due to its favorable conduction band potential, lower electron effective mass, and reduced charge carrier recombination [52,53]. Conductive substrates such as fluorine-doped tin oxide (FTO), indium-doped tin oxide (ITO), or metallic foils (e.g., titanium) enhance electron extraction and facilitate efficient charge transport [54,55]. Optimizing the semiconductor–substrate interface is essential for minimizing interfacial resistance and ensuring rapid charge transport, and this can be achieved via surface treatments, interfacial engineering, or the introduction of buffer layers.

Application of an external anodic bias leads to the formation of a space charge region (depletion layer) at the TiO₂–electrolyte interface, establishing an internal electric field that promotes directional charge carrier migration. The optimal bias voltage is closely related to the flat-band potential of TiO₂ and typically ranges between 0.5 and 1.5 V vs. Ag/AgCl reference electrode [56,57]. An inadequate bias may fail to provide sufficient driving force for charge separation, whereas an excessively high potential may initiate competing electrochemical side reactions that compromise the overall photoelectrocatalytic performance.

Real-time and operando spectroscopic analyses have yielded important mechanistic insights into interfacial charge dynamics during photoelectrocatalysis [58]. Ultrafast time-resolved measurements reveal that electron transfer from TiO₂ to the conductive substrate occurs on the femtosecond to picosecond scale, while hole transfer to surface-adsorbed species typically transpires over nanoseconds to microseconds [59,60]. This disparity in transfer kinetics underscores the necessity of efficient charge separation strategies to minimize recombination losses and prolong charge carrier lifetimes.

Real-time and operando characterization techniques offer critical insights into PEC interface dynamics and redox processes. In situ Raman and ATR-FTIR spectroscopy enable monitoring of intermediates during CO₂ reduction or organic pollutant oxidation, while XPS and XAS under bias elucidate oxidation state changes and surface composition.

Selectivity modulation during PEC can be achieved by tuning the surface structure, doping profile, or integrating co-catalysts. For instance, Cu- or Ni-modified TiO₂ not only improves charge transfer but also alters the product distribution in CO₂ reduction, favoring formate or methanol pathways. In wastewater systems, controlled oxidation of targeted contaminants may be directed by defect engineering or selective adsorption facilitated by surface functional groups.

2.3. Formation of Reactive Oxygen Species

The oxidative capacity of TiO₂-based PEC systems is largely attributable to the generation of ROS, including hydroxyl radicals (•OH), superoxide radicals (O₂•⁻), singlet oxygen (¹O₂), and hydrogen peroxide (H₂O₂) [61,62]. Hydroxyl radicals, generated predominantly by oxidation of water or hydroxide ions at the TiO₂ surface, possess a high oxidation potential (+2.8 V vs. NHE) and effectively mineralize organic pollutants [63,64]. Superoxide radicals, formed via conduction band electrons reducing molecular oxygen, contribute to pollutant degradation by producing additional ROS, such as H₂O₂ [65,66].

Hydrogen peroxide can be further activated by photogenerated electrons or UV irradiation, yielding additional hydroxyl radicals. Singlet oxygen, though less extensively studied, forms through energy transfer or secondary ROS reactions, selectively degrading certain electron-rich pollutants [67].

2.4. Reaction Kinetics and Degradation Pathways

Organic pollutant degradation kinetics in TiO₂ PEC generally follow the Langmuir–Hinshelwood (L–H) model, accounting for pollutant adsorption and subsequent oxidative surface reactions [68,69]. At dilute pollutant concentrations, kinetics simplify to pseudo-first-order behavior. Oxidative degradation initiates with hydroxyl radical attacks on electron-rich functional groups, forming hydroxylated intermediates, which subsequently undergo ring-opening and further oxidation to short-chain organic acids, ultimately mineralizing into CO₂ and H₂O. An illustrative example is the degradation of bisphenol A, involving sequential hydroxylation, oxidative ring cleavage, and mineralization, demonstrating the effectiveness of PEC for detoxifying complex organic pollutants [70]. As shown in Figure 4 [71], under solar irradiation, photoexcited electrons and holes are separated and participate in surface reactions.

As illustrated in Figure 4, the photoelectrocatalytic (PEC) degradation mechanism involves several key processes. Upon visible light irradiation (hv), electrons (e⁻) are excited from the valence band (VB) to the conduction band (CB), generating electron–hole pairs (e⁻/h⁺). Metal doping facilitates charge separation by acting as electron or hole traps and reduces recombination losses. The photogenerated holes (h⁺) at the VB participate in the oxidation of water or hydroxide ions to form hydroxyl radicals (•OH), while the excited electrons (e⁻) reduce oxygen to superoxide radicals (O₂•⁻). These reactive oxygen species (ROS) are responsible for the non-selective mineralization of organic pollutants into CO₂ and H₂O.

2.5. Factors Affecting TiO₂ Photoelectrocatalytic Efficiency

The overall performance of TiO₂-based PEC systems is influenced by intrinsic material properties and operational parameters, including crystalline phase composition, film thickness, external bias, illumination conditions, electrolyte pH, and inorganic ions. Anatase–rutile composites, notably commercial P25 (approximately 80% anatase and 20% rutile), typically exhibit superior PEC performance due to enhanced interfacial charge separation [72]. Optimal TiO₂ film thickness balances photon absorption efficiency with minimal recombination [73]. Applied external bias significantly influences charge carrier separation and recombination, with excessive potentials potentially triggering unwanted side reactions [74]. Light intensity and wavelength dictate electron–hole generation rates; unmodified TiO₂ requires ultraviolet excitation unless engineered for visible-light activation [75]. Electrolyte pH modulates surface charge, pollutant adsorption, and ROS generation; acidic conditions favor pollutant adsorption, whereas alkaline conditions enhance hydroxyl radical formation. Inorganic ions, such as phosphate and carbonate, may act as ROS scavengers, whereas chloride ions can form reactive chlorine species, potentially assisting pollutant degradation [76]. A comprehensive understanding of these parameters is essential to optimize TiO₂ PEC systems, enhancing their applicability for practical environmental remediation.

3. TiO₂ Modification Strategies for Enhanced Visible Light Response

Although TiO₂ exhibits numerous desirable properties—such as high intrinsic photocatalytic activity, excellent chemical stability, non-toxicity, and cost-effectiveness—its practical application in photoelectrocatalysis is largely limited by two intrinsic limitations: (1) a wide bandgap (3.0–3.2 eV), which restricts its photoactivity to the ultraviolet (UV) region, accounting for only ~5% of the solar spectrum, and (2) the rapid recombination of photogenerated electron–hole pairs, which significantly reduces quantum efficiency [26]. To overcome these limitations and extend its photoresponse into the visible region, a variety of modification strategies have been proposed. This section provides a comprehensive overview of these approaches, including elemental doping, defect engineering, heterojunction construction, and the exploitation of surface plasmon resonance (SPR) effects.

3.1. Doping Strategies

Doping refers to the intentional introduction of foreign atoms into the TiO₂ lattice to alter its electronic band structure and enhance its light-harvesting and charge-transport characteristics. Based on the dopant species, doping strategies are generally categorized into metal and non-metal doping.

3.1.1. Metal Doping

Metal doping involves the incorporation of metal ions into the TiO₂ crystal lattice, either substitutionally (replacing Ti⁴⁺ ions) or interstitially. Metal dopants can introduce mid-gap energy levels, thereby enabling the absorption of visible light and facilitating interband electronic transitions [77]. Furthermore, certain metal ions such as Fe and Ag not only enhance visible-light absorption but also facilitate charge separation and reactive oxygen species generation. The overall photocatalytic mechanism of the Fe and Ag co-doped TiO₂/AC system is illustrated in Figure 5 [78]. Density of states (DOS) calculations and EELS spectra indicate that doping with B and N introduces mid-gap states, narrows the bandgap, and modifies the electronic structure of TiO₂. The schematic diagram further illustrates the band alignment and energy transitions resulting from core–shell doping structures.

Among transition metals, cerium (Ce) doping has shown considerable promise. For example, Ce-doped TiO₂ photoanodes have demonstrated enhanced performance in the photoelectrocatalytic reduction of CO₂ to C₂ products under visible light [79]. The incorporation of Ce⁴⁺ not only narrows the bandgap via intermediate states but also functions as an electron trap, facilitating charge separation. A Faradaic efficiency of up to 68% for ethanol and acetate production was achieved, highlighting the dual role of Ce in light absorption and charge management.

Similarly, cobalt (Co) doping in ZnO lattices has been explored to extend light absorption into the visible region. Substitution of Zn²⁺ with Co²⁺ introduces intra-bandgap states, enhancing visible light harvesting and improving photocatalytic performance. Compared to Ag–ZnO photoanodes, Zn_1−xCo_xO systems exhibited superior photoelectrocatalytic activity owing to more effective charge separation and enhanced light absorption [80].

Noble metal doping—particularly with Pd, Pt, and Au—provides additional benefits via multiple mechanisms. These metals can serve as electron sinks, promote interfacial charge transfer through Schottky junction formation, and induce localized surface plasmon resonance (LSPR), which enhances visible light absorption. For instance, Pd-decorated ZnO photoanodes have demonstrated improved degradation of paracetamol under visible light, attributed to LSPR-induced light absorption and efficient electron–hole separation facilitated by Schottky barriers at the Pd–ZnO interface [81].

Nonetheless, excessive doping concentrations may lead to the formation of recombination centers or disrupt lattice periodicity, thereby reducing photocatalytic efficiency. Therefore, careful optimization of dopant type and concentration is essential to balance light absorption and carrier transport.

3.1.2. Non-Metal Doping

Non-metal doping entails the incorporation of light elements—such as nitrogen (N), carbon (C), sulfur (S), boron (B), and fluorine (F)—into the TiO₂ lattice, often substituting for lattice oxygen. These dopants modulate the valence band structure by introducing impurity states or hybridizing their p orbitals with O 2p states, thereby narrowing the bandgap and enabling visible light activation [29].

Nitrogen doping is among the most extensively investigated non-metal doping strategies. N-doped TiO₂ exhibits a notable red shift in its absorption spectrum, attributable to the introduction of N 2p states above the valence band maximum, which reduces the effective bandgap. For instance, N-doped TiO₂ photoanodes have shown enhanced degradation of methylene blue under visible light, outperforming pristine TiO₂, which remains inactive under the same conditions [82].

Sulfur doping has also demonstrated efficacy in extending the photoresponse into the visible region. The incorporation of S 3p orbitals into the TiO₂ valence band reduces the bandgap and promotes light absorption. For example, S-doped Mn–TiO₂ photoanodes exhibited enhanced degradation of ribavirin under visible light, owing to the synergistic effects of S-induced bandgap narrowing and Mn-facilitated charge separation [83].

Carbon doping, another widely explored strategy, can occur via substitutional or interstitial incorporation, or through surface modification with carbonaceous species such as carbon quantum dots (CQDs). C-doped TiO₂ exhibits red-shifted absorption spectra, improved carrier separation, and enhanced photoelectrocatalytic activity. CQD-modified TiO₂, in particular, has demonstrated superior performance due to the dual role of CQDs in expanding light absorption and facilitating electron transfer via their excellent electron-accepting capabilities [84].

Co-doping with multiple non-metallic elements has emerged as a promising approach for synergistic bandgap modulation and charge separation enhancement. For example, N,S-co-doped TiO₂ has been shown to outperform singly doped counterparts in both light absorption and photoelectrocatalytic efficiency under visible light, owing to improved orbital hybridization and extended carrier lifetimes [85].

It is essential to distinguish between lattice doping and surface decoration of TiO₂. Doping involves the incorporation of atoms such as Ag, Fe, or N into the TiO₂ lattice—either substitutionally or interstitially—which alters the band structure, creates mid-gap states, and modifies charge carrier behavior. In contrast, surface decoration refers to the deposition of nanoparticles or thin films of foreign materials (e.g., Ag, Pd) that form interfaces or Schottky junctions without entering the TiO₂ lattice.

For example, Ag-decorated TiO₂ exhibits enhanced visible-light activity due to surface plasmon resonance and interfacial charge transfer, which is different from Ag doping where the metal acts as an electron sink within the lattice. Similarly, nitrogen-doped TiO₂ (N–TiO₂) shows enhanced electrochemical activity even under dark conditions, owing to electronic structure modification and improved conductivity.

According to recent findings, excessive dopant concentrations (>3 at.%) may introduce recombination centers that adversely affect photocatalytic efficiency. Hence, most high-performing systems optimize doping within the 0.5–2 at.% range [86].

3.2. Defect Engineering

Defect engineering entails the deliberate manipulation of crystal imperfections within the TiO₂ lattice to tailor its electronic structure, optical absorption characteristics, and photoelectrocatalytic performance. These defects can be broadly categorized into intrinsic types—such as oxygen vacancies and titanium interstitials—and extrinsic types, including dopant-induced lattice distortions and surface imperfections. Among them, oxygen vacancies have garnered the most attention due to their pronounced impact on visible light absorption and charge carrier dynamics.

Oxygen vacancies act as shallow donor states, introducing mid-gap energy levels that extend the optical absorption edge of TiO₂ into the visible spectrum [30]. In addition to enhancing light absorption, these vacancies increase carrier concentration and conductivity by acting as electron donors. Moreover, they serve as electron trapping sites, thereby facilitating charge separation and suppressing bulk recombination. Various methodologies have been employed to generate oxygen vacancies in TiO₂, including thermal annealing in reducing atmospheres, hydrogenation, plasma exposure, and chemical reduction processes.

Surface defect engineering via acid treatment has also been shown to significantly improve the PEC performance of TiO₂. For example, hydrofluoric acid (HF) treatment of TiO₂ nanotubes resulted in increased concentrations of surface oxygen vacancies, which enhanced visible light absorption and improved interfacial charge separation [87]. The treated nanotubes exhibited a 2.5-fold increase in the degradation rate of methylene blue compared to their pristine counterparts—an improvement attributed to the synergistic effects of light absorption and defect-induced charge management.

Furthermore, three-dimensional titanium substrates supporting TiO₂ nanotube arrays have been reported to induce a higher density of interface-specific defects, particularly at the nanotube–substrate junction. This architectural configuration promotes superior charge transport and spatial separation of photogenerated carriers, yielding enhanced PEC activity relative to conventional two-dimensional arrays [88].

Nevertheless, it is essential to note that an excessive concentration of defects may act as deep-level recombination centers, ultimately diminishing photocatalytic performance. Thus, fine-tuning the defect density and distribution is critical for maximizing PEC efficiency.

3.3. Heterojunction Construction

Constructing heterojunctions by coupling TiO₂ with other semiconductors offers an effective strategy to enhance light absorption, suppress charge recombination, and promote interfacial charge transfer. Depending on the relative band alignment of the constituent semiconductors, heterojunctions are commonly classified into three types: Type I (straddling gap), Type II (staggered gap), and Type III (broken gap). Among these, Type II heterojunctions are most widely employed in PEC systems due to their efficient charge separation behavior.

3.3.1. TiO₂-Based p–n Heterojunctions

p–n heterojunctions are formed by interfacing n-type TiO₂ with p-type semiconductors, such as Cu₂O, CuO, NiO, and BiOX (X = Cl, Br, I). The built-in electric field at the junction interface facilitates the spatial separation of photogenerated charge carriers—electrons migrate toward the n-type region, while holes are directed toward the p-type domain—thereby suppressing recombination and enhancing PEC activity [89].

However, conventional p–n junctions formed by TiO₂ and simple metal oxides often exhibit limited carrier mobility and recombination suppression. Hence, more sophisticated designs are needed. A rationally engineered p–n heterojunction comprising n-type BaTiO₃ and p-type NiO was constructed to enhance charge separation efficiency through interfacial band alignment and piezoelectric modulation (Figure 6) [90]. The Mott–Schottky analysis revealed negative and positive slopes for BaTiO₃ and NiO, respectively, confirming their n- and p-type semiconductor nature, with flat-band potentials of −1.14 V and 1.48 V (vs. Ag/AgCl), respectively. Upon contact, a staggered Type II band alignment is formed, with electrons migrating from BaTiO₃ to NiO and holes moving in the opposite direction. The built-in electric field at the interface facilitates spatial charge separation, while the ferroelectric polarization of BaTiO₃ further enhances the internal electric field, enabling more efficient carrier migration. This synergistic effect is anticipated to significantly improve photocatalytic or piezocatalytic performance by reducing recombination and enhancing interfacial charge transport.

Similarly, a ferroelectric-enhanced BiVO₄/BiFeO₃ p–n heterojunction demonstrated superior performance for the photoelectrocatalytic degradation of tetracycline [91]. The spontaneous polarization of BiFeO₃ contributed an internal electric field that further assisted charge dissociation at the junction, highlighting the benefit of integrating ferroelectric components into PEC architectures.

Beyond p–n and conventional Z-scheme heterojunctions, heterojunctions formed between similar wide-bandgap semiconductors, such as TiO₂–WO₃ and TiO₂–SnO₂, have been demonstrated to significantly improve charge carrier separation while maintaining strong oxidative potentials. These Type II alignments enable directional electron flow from TiO₂ to WO₃, leveraging their differential conduction band energies to suppress recombination and extend activity into the visible region.

3.3.2. TiO₂-Based Z-Scheme Heterojunctions

Z-scheme heterojunctions are bioinspired architectures that emulate the natural photosynthetic electron transfer chain. They couple two semiconductors via a solid-state electron mediator or direct interface contact, allowing photogenerated electrons from one semiconductor to recombine with holes from the other. This configuration retains the strong redox potential of each component and promotes spatial charge separation [92].

Another sophisticated example is the multi-interface polarization-engineered 1T–2H MoS₂/TiO₂ Z-scheme system (Figure 7) [93]. The internal phase boundaries between metallic 1T and semiconducting 2H MoS₂ phases created localized electric fields, which, in conjunction with the TiO₂ interface, reinforced charge separation. The system exhibited superior PEC performance under visible light, affirming the advantages of engineered interfacial polarization.

3.3.3. TiO₂-Based Carbon Material Heterojunctions

The integration of TiO₂ with conductive carbonaceous materials—such as graphene, carbon nanotubes (CNTs), and CQDs—has emerged as a promising approach to enhance PEC performance by improving charge carrier dynamics and light absorption [94]. Carbon materials act as electron acceptors, facilitating directional charge transfer and mitigating recombination. Additionally, their high conductivity and surface area contribute to improved photon utilization and electrolyte interaction.

Two-dimensional graphitic materials, particularly graphene and its derivatives, have been widely employed to construct TiO₂-based heterojunctions [95]. The exceptional electrical conductivity, large specific surface area, and mechanical flexibility of graphene promote efficient electron transport and extended light harvesting. Graphene–TiO₂ composites have demonstrated enhanced degradation of organic dyes under visible light due to improved charge carrier separation and sensitization effects.

Mechanistic studies on graphene–TiO₂ photoanodes revealed that graphene serves as an efficient electron sink, accepting electrons from the TiO₂ conduction band and preventing their recombination with photogenerated holes [96].

More advanced architectures, such as hierarchical TiO₂ nanowire arrays grown on graphite fibers, have been shown to further enhance interfacial contact and charge separation [97]. The graphite fiber substrate acts as an efficient electron collector, facilitating rapid carrier extraction and reducing recombination, resulting in significantly improved pollutant degradation.

3.3.4. TiO₂–WO₃ Heterojunctions for Visible-Light Activation

Heterojunctions formed between similar wide-bandgap semiconductors, such as TiO₂ and WO₃, have been extensively studied due to their favorable band alignment and charge transfer properties. WO₃ possesses a smaller bandgap (~2.7 eV) and a more positive conduction band edge compared to TiO₂. When coupled, electrons excited in TiO₂ transfer to WO₃, while holes remain in TiO₂, forming a Type II heterojunction that facilitates charge separation and extends the photocatalytic activity into the visible light region. Several studies have demonstrated that TiO₂–WO₃ composites show significantly enhanced photocatalytic degradation of dyes and organic pollutants under simulated solar irradiation, compared to bare TiO₂ [23,49].

Such systems represent a practical strategy to overcome TiO₂’s intrinsic UV-only limitation and provide a platform for visible-light-driven PEC applications.

3.4. Surface Plasmon Resonance Effects

Surface plasmon resonance (SPR) refers to the coherent oscillation of conduction band electrons at the interface between a metal nanoparticle and a dielectric medium when irradiated with light at a resonant frequency. SPR-active nanostructures can significantly enhance the photoelectrocatalytic (PEC) performance of TiO₂ via several mechanisms, including (i) local electromagnetic field enhancement, (ii) hot electron injection into the semiconductor, and (iii) broadening of the light absorption spectrum into the visible region.

3.4.1. Noble Metal Plasmonics

Noble metals such as Au, Ag, and Pt exhibit strong SPR phenomena in the visible spectrum, making them highly effective in extending the photoresponse of TiO₂. Upon photoexcitation, the SPR-induced hot electrons in these metals can be transferred to the conduction band of TiO₂, thereby initiating redox reactions under visible light.

For instance, Ag-decorated V₂O₅–TiO₂ nanocomposites have exhibited remarkable PEC activity for organic pollutant degradation under visible light [98]. The localized SPR of Ag nanoparticles not only enhanced photon absorption but also facilitated hot electron injection into the TiO₂ conduction band. As a result, the plasmonic system demonstrated a 4.1-fold increase in methylene blue degradation compared to pristine TiO₂.

Similarly, Ag–ZnO photoanodes have shown enhanced PEC efficiency due to SPR-assisted charge separation [80]. In this system, Ag nanoparticles served as both light-harvesting centers and electron donors, thereby improving visible light utilization and carrier mobility.

3.4.2. Non-Noble Metal Plasmonics

To mitigate the cost and scarcity of noble metals, significant efforts have been directed toward exploring non-noble metal plasmonic materials—such as Cu, Al, and transition metal nitrides—that exhibit SPR-like behavior in the visible and near-infrared regions [99].

Copper-based plasmonic TiO₂ photocatalysts have shown promising results for the degradation of organic pollutants under solar irradiation. Cu nanoparticles deposited on TiO₂ surfaces introduced visible light activity via SPR, while simultaneously improving charge separation through hot electron transfer mechanisms. The Cu–TiO₂ system outperformed pristine TiO₂ under comparable irradiation conditions, demonstrating its potential as a cost-effective plasmonic alternative.

3.4.3. Synergistic Plasmonic–Semiconductor Hybrid Systems

Integrating SPR-active materials with other modification strategies—such as elemental doping and heterojunction engineering—can yield synergistic effects that substantially enhance PEC performance.

For example, Ag-decorated N-doped TiO₂ systems have demonstrated superior PEC activity under visible light compared to their individually modified counterparts [100]. The synergistic effect arises from the combination of SPR-induced hot electron generation (from Ag) and bandgap narrowing (from nitrogen doping), both of which contribute to improved light absorption and charge transport.

Similarly, Ag nanoparticle-decorated TiO₂–graphene heterojunctions have shown notable performance enhancements due to dual mechanisms: plasmonic excitation and interfacial charge transfer [31]. The interfacial synergy between the TiO₂ semiconductor, graphene electron conductor, and Ag plasmonic sensitizer resulted in significantly improved pollutant degradation under visible light.

3.5. Other Modification Strategies

Beyond the widely investigated strategies, several emerging modification approaches have been developed to further expand the visible light activity of TiO₂-based PEC systems.

3.5.1. Conductive Polymer Functionalization

Conductive polymers—including polyaniline (PANI), polypyrrole (PPy), and poly(3,4-ethylenedioxythiophene) (PEDOT)—offer tunable optoelectronic properties and have been successfully incorporated into TiO₂-based materials to extend light absorption and improve interfacial charge transport.

For instance, electrically conductive TiO₂–PANI–PVDF composite membranes have shown significantly improved PEC degradation of organic pollutants under visible light (Figure 8) [101]. The incorporation of PANI enhanced light absorption and facilitated electron transport, owing to its π-conjugated structure and favorable energy alignment with TiO₂. Similarly, PEDOT-modified PVDF membranes embedded with TiO₂ nanoparticles exhibited a 2.8-fold improvement in methylene blue degradation efficiency, attributed to improved conductivity and enhanced charge separation.

3.5.2. Organic Dye Sensitization

Dye sensitization is a classical strategy adapted from dye-sensitized solar cells (DSSCs), wherein organic dyes adsorbed onto TiO₂ surfaces absorb visible light and inject excited electrons into the TiO₂ conduction band. This expands the spectral response of TiO₂ into the visible region, enabling PEC reactions under solar irradiation.

Various dyes—including ruthenium complexes, porphyrins, and natural pigments—have been employed to sensitize TiO₂. N719-sensitized TiO₂ photoanodes, for example, exhibited marked improvements in PEC degradation of methylene blue under visible light, in contrast to the negligible activity of unmodified TiO₂ [36].

3.5.3. Coupling with Energy Harvesting Systems

The integration of TiO₂ PEC systems with self-powered energy harvesting devices—such as triboelectric and piezoelectric nanogenerators—has emerged as a cutting-edge approach for enhancing performance and energy autonomy.

To achieve a fully self-powered photoelectrochemical (PEC) system, we integrated a rotational electromagnetic energy harvester with the photoanode module. This device converts mechanical energy into electrical energy in real time, enabling bias-free PEC reactions under ambient conditions. A representative system combining a triboelectric–electromagnetic nanogenerator with a TiO₂-based Type II heterojunction was demonstrated for water treatment applications (Figure 9) [102]. Mechanical energy harvested from water flow was converted into electrical energy, which provided an external bias to drive charge separation in the PEC system. The self-powered configuration showed significantly enhanced degradation of pollutants, even under low light intensity conditions, underscoring the potential of hybrid energy–catalysis platforms.

Collectively, these diverse modification strategies offer promising routes for overcoming the intrinsic limitations of TiO₂, particularly its wide bandgap and rapid charge recombination. Through synergistic integration of multiple enhancement approaches—such as doping, heterojunction engineering, plasmonic sensitization, and hybrid coupling with functional materials—TiO₂-based PEC systems can achieve substantially improved performance under visible light irradiation. Continued advancements in material design, interface engineering, and system integration will be critical to translating laboratory-scale innovations into scalable solutions for solar-driven environmental remediation.

4. Environmental Applications of TiO₂-Based Photoelectrocatalysis

TiO₂-based photoelectrocatalysis (PEC) has garnered increasing attention as a promising solution to various environmental issues, particularly in the context of advanced water and wastewater treatment. By combining photocatalytic oxidation with electrochemical bias-induced charge separation, TiO₂-based systems exhibit superior pollutant degradation efficiency and enhanced operational robustness. The integration of advanced material modifications—such as doping, heterojunction construction, and plasmonic enhancement—further broadens their applicability. This section highlights key environmental applications of TiO₂-based PEC, with an emphasis on the degradation of organic contaminants, disinfection, and coupled energy conversion processes.

4.1. Organic Pollutant Degradation

The removal of persistent organic pollutants (POPs) constitutes one of the most widely explored applications of TiO₂-based PEC. Compared with conventional treatment technologies, PEC offers several distinct advantages: high redox potential, non-selective reactivity, and the capability for complete mineralization of contaminants into CO₂ and H₂O.

4.1.1. Pharmaceutical Compounds

Pharmaceuticals, including antibiotics, analgesics, and endocrine disruptors, are frequently detected in aquatic systems due to widespread consumption, partial human metabolism, and limited removal efficiency in conventional wastewater treatment plants. TiO₂-based PEC systems have demonstrated remarkable potential in degrading such micropollutants under controlled conditions.

For instance, paracetamol (acetaminophen), a widely consumed analgesic, has been efficiently degraded using TiO₂ photoanodes [103]. Comparative studies revealed that PEC achieved a degradation efficiency of 95%, outperforming both photocatalysis (78%) and electrochemical oxidation (65%) under identical conditions. This enhanced performance was attributed to efficient electron–hole separation under external bias, which promoted both direct oxidation by holes and indirect oxidation via hydroxyl radical formation.

Levofloxacin, a fluoroquinolone antibiotic, was also efficiently removed through PEC with TiO₂ photoanodes, achieving >92% degradation within 60 min under UV irradiation and optimized bias (1.0 V, pH 7) (Figure 10) [104]. The degradation kinetics followed a pseudo-first-order model, driven by hydroxyl radical attack on the aromatic ring system.

Figure 10 provides essential electrochemical evidence supporting the PEC performance. Figure 10d shows the relationship between capacitive current and scan rate, which was used to estimate the electrochemical surface area (ECSA) via double-layer capacitance analysis. This value reflects the number of electroactive sites available for surface reactions during the PEC process. Figure 10c, derived from linear sweep voltammetry (LSV), illustrates the photocurrent response as a function of applied potential, indicating the PEC activity and identifying the onset potential of photocurrent generation. Moreover, the Nyquist plot in Figure 10d, obtained from electrochemical impedance spectroscopy (EIS), reveals a reduced charge transfer resistance under illumination, indicating improved interfacial charge transport and enhanced photoelectrochemical kinetics.

In addition to ECSA, other methodologies for assessing the active surface area include Brunauer–Emmett–Teller (BET) surface area analysis, transient photocurrent response measurements, and incident photon-to-current efficiency (IPCE) mapping. These complementary techniques can provide a more comprehensive understanding of surface properties and photoelectrochemical performance.

4.1.2. Dyes and Pigments

Synthetic dyes—such as azo, anthraquinone, and triphenylmethane compounds—are prevalent in industrial effluents and are known for their high stability and toxicity. PEC treatment offers an effective approach for the breakdown of these chromophores.

A study on the degradation of methylene blue (cationic) and Congo red (anionic) revealed that electrostatic interactions with the TiO₂ surface play a critical role [105]. At near-neutral pH, the negatively charged TiO₂ surface facilitated the adsorption of cationic species, resulting in higher removal efficiency for methylene blue.

4.1.3. Pesticides and Herbicides

The widespread use of agrochemicals has led to frequent contamination of natural water bodies with toxic pesticides and herbicides. TiO₂-based PEC systems have shown efficacy in degrading structurally diverse compounds such as atrazine, 2,4-D, and chlorpyrifos.

In the case of atrazine, TiO₂ nanotube arrays achieved 98% degradation within 120 min under acidic conditions (pH 3) and a 2.0 V bias [106]. The process followed pseudo-first-order kinetics and was governed primarily by •OH-mediated oxidative attack on the triazine ring.

For 2,4-dichlorophenoxyacetic acid (2,4-D), PEC treatment using TiO₂ nanotubes under a 1.5 V bias significantly enhanced removal efficiency compared to photocatalysis alone [107]. Identified intermediates indicated successive dechlorination and oxidation steps, again emphasizing the central role of hydroxyl radicals in pollutant breakdown.

4.1.4. Industrial Chemicals

Industrial effluents typically contain complex mixtures of phenols, halogenated organics, and other recalcitrant aromatic compounds. The non-selective oxidative capability of TiO₂-based PEC systems makes them ideal for treating such wastewater.

For example, the mineralization of phenol was significantly improved by coupling PEC with ozonation, achieving 95% total organic carbon (TOC) removal, compared to 78% and 65% for standalone PEC and ozonation, respectively [108]. The synergy was attributed to the generation of additional •OH radicals via ozone–electron interactions.

In another study, reduced graphene oxide (rGO)-modified TiO₂ photoanodes facilitated enhanced degradation of p-chloronitrobenzene, a persistent industrial pollutant [109]. The incorporation of rGO extended visible light absorption and improved electron mobility, resulting in 92% degradation within 60 min under visible light—compared to only 45% with unmodified TiO₂.

These findings collectively demonstrate the versatility of TiO₂-based PEC systems in addressing a wide range of organic contaminants. Through careful control of operational parameters (e.g., pH, bias potential) and material modifications (e.g., nanotube structures, carbon-based composites), high-efficiency degradation can be achieved even for structurally complex and recalcitrant pollutants.

4.2. Water Treatment and Disinfection

In addition to the degradation of organic pollutants, TiO₂-based photoelectrocatalysis (PEC) has exhibited considerable potential in broader water treatment applications, including heavy metal removal, microbial inactivation, and the remediation of industrial wastewaters. The synergistic combination of photocatalysis and electrochemical reduction/oxidation processes enables spatially resolved redox reactions, facilitating the concurrent removal of diverse contaminants.

4.2.1. Heavy Metal Removal

Heavy metals such as chromium, lead, mercury, and cadmium are of environmental concern due to their high toxicity, persistence, and bio accumulative nature. TiO₂-based PEC enables their removal primarily through reductive transformation at the photocathode.

For example, efficient removal of Cr(VI) from tannery wastewater was achieved using TiO₂ photoelectrodes, with a reported reduction efficiency of 99% within 60 min under acidic conditions (pH 3, 1.0 V bias, UV light) [110]. The mechanism involved photogenerated electron-induced reduction of Cr(VI) to Cr(III), followed by precipitation as Cr(OH)₃ at elevated pH.

Interestingly, Cr(VI) itself can function as an electron scavenger in PEC systems, enhancing charge separation by capturing photogenerated electrons and thereby promoting oxidative degradation of co-existing organic pollutants [111]. This dual role of Cr(VI) contributes to a synergistic removal effect in complex wastewater matrices.

Simultaneous removal of methylene blue (95%) and Cr(VI) (98%) under solar irradiation within 90 min has also been demonstrated [112]. This dual functionality underscores the advantage of PEC systems in spatially decoupling oxidation (at the photoanode) and reduction (at the cathode) processes.

4.2.2. Disinfection and Microbial Inactivation

Microbial contamination, including pathogenic bacteria, viruses, and protozoa, poses a serious public health risk. PEC disinfection provides an advanced alternative to traditional chlorination, offering pathogen inactivation without harmful byproducts.

Capacitive TiO₂ photoanodes operated under external bias have shown significantly improved bactericidal performance, attributed to enhanced charge separation and the generation of reactive oxygen species (ROS), including hydroxyl radicals and singlet oxygen [113]. These ROS induce oxidative damage to microbial membranes and intracellular components, leading to cell lysis.

4.2.3. Treatment of Complex Wastewaters

Industrial wastewaters often exhibit high chemical oxygen demand (COD), contain diverse organic and inorganic pollutants, and are challenging to treat via conventional means. TiO₂-based PEC, due to its strong oxidizing power and non-selectivity, is well-suited for these applications.

For instance, a COD removal efficiency of 85% was achieved from gas field produced water within 120 min using TiO₂ nanotube array photoanodes under 2.0 V bias and UV irradiation [114]. The efficacy was primarily driven by in situ generation of ROS that oxidized a broad spectrum of organic constituents.

4.3. Energy Conversion Applications

In addition to environmental remediation, TiO₂-based PEC systems offer opportunities for solar-driven energy conversion, particularly in CO₂ reduction to value-added fuels and hydrogen evolution through water splitting. These applications align with the dual goals of environmental sustainability and renewable energy production.

4.3.1. CO₂ Reduction

The photoelectrocatalytic reduction of CO₂ to fuels or commodity chemicals addresses both carbon neutrality and energy security. TiO₂ photoanodes, when appropriately modified, have shown promising activity for CO₂ conversion under visible light.

A Cu-modified TiO₂ system achieved a Faradaic efficiency of 85% for formate production under visible light, attributed to efficient charge separation and Cu-mediated CO₂ reduction catalysis [115]. The presence of Cu facilitated multi-electron transfer processes and stabilized CO₂ intermediates on the electrode surface.

4.3.2. Water Splitting for Hydrogen Generation

PEC water splitting for hydrogen production is an attractive pathway for sustainable energy conversion. TiO₂-based systems utilize photogenerated holes for water oxidation at the photoanode and electrons for proton reduction at the cathode. TiO₂ has served as the cornerstone of PEC water splitting research since the seminal Honda–Fujishima discovery in 1972. Despite its outstanding photostability, its wide bandgap limits solar spectrum utilization, necessitating intensive modification efforts. Recent advancements, including cocatalyst loading and heterojunction engineering, have notably improved its hydrogen evolution efficiency under visible light [116].

In a study, a TiO₂ PEC system was employed for the dual purpose of alcohol oxidation and hydrogen generation, achieving Faradaic efficiencies of 92% for aldehyde formation and 95% for H₂ evolution under UV light and 0.6 V bias [117]. This dual-function platform demonstrates the feasibility of coupling selective organic transformations with clean energy production.

TiO₂-based photoelectrocatalysis represents a versatile platform that integrates pollutant degradation with energy conversion. Through rational material design and system-level integration, significant advancements have been achieved in contaminant removal, pathogen inactivation, and solar-to-chemical energy transformation. Nevertheless, further work is required to address challenges related to selectivity, long-term stability, and scale-up for real-world applications—issues that will be explored in the following section.

4.3.3. Photoelectrolysers and Photofuel Cells for Simultaneous Remediation and Energy Generation

An emerging trend in photoelectrocatalysis is the development of dual-function systems that simultaneously degrade pollutants and generate energy. Known as photoelectrolysers or photofuel cells, these systems utilize organic wastewater as a sacrificial electron donor to produce hydrogen or electricity, thus achieving both environmental and energetic objectives [117].

Lianos et al. first conceptualized the photofuel cell, where PEC oxidation of organics is coupled to cathodic oxygen reduction or hydrogen evolution. More recently, PEC platforms employing TiO₂ nanotubes, doped oxides, or plasmon-enhanced materials have shown promise for both pollutant mineralization and hydrogen generation under solar light [118].

This integrated approach contributes to sustainability by valorizing waste streams into useful energy carriers.

4.4. Gas-Phase PEC Systems with Proton Exchange Membranes (PEMs)

Gas-phase photoelectrocatalytic systems integrated with proton exchange membranes (PEMs) offer a unique configuration for decentralized pollutant treatment and solar-driven fuel production. These systems eliminate the need for bulk liquid electrolytes and allow for more efficient mass transfer in humidified gas environments. Einaga and co-workers have demonstrated boron-doped diamond (BDD)-based PEM devices capable of gas-phase water splitting and degradation of volatile organic compounds. Similarly, Tsampas and Chatzitakis have advanced the design of gas-diffusion photoanodes integrated with Nafion membranes for the selective reduction of CO₂ and simultaneous H₂ production [42].

The main advantages of these devices include scalability, reduced ionic resistance, and integration potential with solar PV modules. However, challenges such as membrane durability, gas permeation control, and catalyst deactivation under dry conditions require further research.

5. Challenges and Future Prospects

5.1. Efficiency and Visible Light Utilization

TiO₂’s intrinsic wide bandgap (3.0–3.2 eV) restricts its photoresponse to the UV spectrum, which accounts for less than 5% of solar radiation. Although doping, heterojunction construction, and surface plasmon resonance (SPR) have broadened its visible light activity, the overall solar-to-chemical conversion efficiency remains relatively low [119].

Future efforts should focus on constructing multi-component hybrid systems with optimized band alignments and interfacial engineering to facilitate visible light harvesting and charge transport. The integration of PEC systems with renewable electricity sources (e.g., solar PV, hydro, wind) to power the external bias represents a practical route to enhance sustainability and reduce fossil energy dependence.

To contextualize PEC development, it is necessary to compare current system performance with international solar fuel benchmarks. According to the U.S. Department of Energy (DOE), practical photoelectrochemical water splitting systems should achieve >10% solar-to-hydrogen (STH) efficiency and >5000 h of operational durability. However, state-of-the-art TiO₂-based systems typically achieve STH efficiencies below 2% under visible light [48].

Recent studies suggest that hybrid architectures, tandem junctions, and interface engineering may help close this gap, though TiO₂ remains fundamentally limited by its wide bandgap. Bridging the performance gap will require multidisciplinary efforts in material synthesis, photophysics, and system integration [116].

5.2. Charge Separation, Transport, and Stability

While external bias improves charge separation, electron–hole recombination and low intrinsic conductivity remain major bottlenecks [120]. Tailoring electrode morphology—such as constructing 1D or 3D nanostructures—and incorporating conductive components like graphene or carbon nanotubes has shown promise [121]. Future research should explore advanced junction architectures (e.g., p–n–p or n–p–n systems) and core–shell designs to further suppress recombination while maintaining durability under operational stress [122].

5.3. Reactor Design and Scale-Up

Most PEC systems remain confined to lab-scale due to limitations in reactor design, light penetration, and electrode fabrication. Flow maldistribution and high energy input for mixing further constrain performance [2]. Novel reactor configurations—such as microfluidic and membrane-based designs—and modular, scalable systems using embroidered or roll-to-roll flexible electrodes show great potential [123]. Coupling computational fluid dynamics (CFD) modeling with experimental optimization will be critical for system-level scale-up.

Recent advances have also explored gas-phase PEC systems integrated with proton exchange membrane (PEM) reactors. These devices operate under continuous flow, enabling selective oxidation of gaseous VOCs and NO_x under ambient conditions. Studies have reported promising results in terms of efficiency, product selectivity, and operational stability, thus expanding PEC applications beyond aqueous systems. Beyond light-driven TiO₂ PEC systems, recent studies have explored non-noble metal electrocatalysts—such as Fe–Ni, Co–Mo, or Ni–Cu bimetallics—for pollutant degradation and hydrogen production under dark conditions. These catalysts offer cost-effective alternatives with high electrochemical activity in nitrate reduction, urea oxidation, and CO₂ electroreduction pathways.

Integrating such catalysts into PEC-electrochemical hybrid systems could provide 24 h operation or improve reaction selectivity in low-light conditions. While this review centers on light-active TiO₂ materials, we acknowledge the growing importance of dark electrocatalysis for water and wastewater treatment, especially in industrial settings where continuous operation is required.

6. Conclusions

This review summarizes recent advancements in TiO₂-based photoelectrocatalysis (PEC), with an emphasis on enhancing visible light utilization and its environmental applications. The integration of photocatalysis with electrochemical bias effectively mitigates electron–hole recombination, improving charge carrier dynamics and catalytic efficiency. Spatially separated redox reactions at the photoanode and cathode enable efficient pollutant degradation and concurrent resource recovery.

Modification strategies, including doping, defect engineering, heterojunctions, and surface plasmon resonance (SPR), have significantly improved TiO₂’s performance by modulating its electronic structure and broadening its absorption spectrum. PEC systems have shown remarkable versatility in the degradation of organic pollutants, heavy metals, and in microbial disinfection, while also facilitating CO₂ reduction and hydrogen evolution.

However, challenges persist, notably in achieving high solar-to-chemical conversion efficiency, enhancing charge separation, ensuring long-term stability, and scaling up PEC reactors. Future research should focus on optimizing composite materials, reactor design, and integrating renewable energy sources, alongside employing advanced characterization and computational models to drive PEC technology toward practical industrial applications.