Open Access Article
Ajith Mohan Arjun
*a,
Menon Ankitha
b,
Manjusha Mathew
c,
Sanjiv Sharma
*a and
P. Abdul Rasheed
*db
aDepartment of Pharmacy and Therapeutics, Institute of Systems, Molecular and Integrative Biology, University of Liverpool, 6 W Derby St., Liverpool L7 8TX, UK. E-mail: arjun.mohan@liverpool.ac.uk; Sanjiv.Sharma@liverpool.ac.uk
bDepartment of Chemistry, Indian Institute of Technology Palakkad, Palakkad, Kerala 678 623, India. E-mail: abdulrasheed@iitpkd.ac.in
cDepartment of Chemistry, Nirmalagiri College, Kuthuparamba, Kannur, Kerala 670701, India
dDepartment of Biological Sciences and Engineering, Indian Institute of Technology Palakkad, Palakkad, Kerala 678 623, India
First published on 11th November 2025
Self-powered electrochemical sensors (SPECSs) offer a transformative alternative by integrating energy harvesting directly with analyte detection, enabling autonomous operation without external power sources. This review focuses on the merits of employing MXenes in the construction and performance of SPECSs by evaluating how MXenes are employed as active components and how they enhance the performance of various SPECS platforms. We broadly classified MXene-based SPECSs as enzymatic biofuel cell-based sensors, microbial- and biophotoelectrochemical-based sensors, and other SPECSs. The key attributes of MXenes, including high conductivity and tunable surface chemistry, are ideal for immobilizing active species in the SPECS. The significant capacitance and catalytic potential of MXenes are explored towards enhancing charge transport in SPECSs. This enables robust interfaces, facilitating signal amplification, and forming advanced functional composites within these self-powered devices. By utilizing these unique properties of MXenes, the development of highly sensitive, stable, and potentially miniaturized autonomous sensors is becoming increasingly feasible, paving the way for next-generation sensing solutions.
The autonomous generation of power in SPECSs directly addresses the significant sustainability challenges posed by conventional sensors. By eliminating the need for external power sources like batteries or solar cells, SPECSs drastically reduce the overall material usage involved in sensor construction. This not only conserves resources but also frees up valuable materials, including precious metals and rare earth elements used in batteries, for other critical applications. Furthermore, many SPECSs, particularly those based on biofuel cells, utilize biomaterials like enzymes and microbes that are more abundant and less environmentally intensive to produce than the components of traditional power sources.4 This reduction in the reliance on resource-intensive, non-renewable materials directly results in a smaller carbon footprint and a more sustainable, self-sufficient sensing platform. This shift marks a move toward a circular economy model for sensors, where the device's operational power is seamlessly integrated with its sensing function, minimizing waste and environmental impact from cradle to grave.
This paradigm shift towards SPEC systems needs to have innovative device designs that are capable of harvesting energy directly from their surroundings or from the electrochemical sensing reaction happening in the system itself. This can be realized by introducing diverse energy conversion strategies integrated directly within the sensor design. The key approaches include (1) harnessing biomechanical energy by using piezoelectric or triboelectric effects to convert vibrations or pressure changes,5 (2) exploiting biochemical reactions similar to enzymatic biofuel cells, where analyte consumption generates current,2 (3) utilizing thermal gradients via thermoelectric generators,6 (4) capturing ambient light through photovoltaic components,7 and (5) converting chemical potential directly into electricity.8 The crucial aspects of design, operation, and potential applications of the sensor are entirely dependent on the selection of the energy harvesting mechanism used in the sensor system. For example, a wearable sensor can utilize the body movement via triboelectric nanogenerators, while an environmental sensor can utilize a biofuel cell powered by pollutants.9 Hence, the sensor design should focus on analyte detection and efficient power generation units in addition to the integration of sensing elements with miniaturized, and operational demands of the sensor.
There are mainly two different approaches such as biofuel cells (BFCs) and photoelectrochemical (PEC) reactions, generally utilized in self-powered electrochemical sensing systems. These systems align with biological and environmental monitoring needs in a way that they generate power directly from metabolites readily available in physiological fluids (like glucose or lactate) in the case of BFCs, or by converting the light energy into PEC systems. A BFC-based self-powered system involves designing a fuel cell electrode with a primary biocatalyst for power generation, and a bioreceptor element that undergoes bioreceptor–analyte interaction, which influences the rate of the power-generating reaction. This can be either enzymatic biofuel cells (EBFCs), which can generate electrical power through highly specific biochemical reactions catalyzed by enzymes immobilized on electrode surfaces or microbial fuel cells (MFCs), which utilize the metabolic activity of electrogenic microorganisms to convert the chemical energy stored in organic matter directly into electricity. These EBFCs show high specificity originating from the enzymatic reactions, making them attractive for detecting particular biomarkers or metabolites.10 In MFCs, changes in the MFC's power output can correlate with fluctuations in the concentration of the microbial substrate (e.g., measuring biochemical oxygen demand in wastewater) or the presence of substances that inhibit or stimulate microbial activity (e.g., toxins).11
For sensors leveraging mechanical (piezoelectric or triboelectric) or thermal energy, the operating principle involves the analyte typically controlling a physical energy conversion process indirectly. In contrast, photoelectrochemical (PEC) systems utilize semiconductor materials (photoelectrodes) that absorb light to generate electron–hole pairs; these charge carriers then drive electrochemical reactions, leading to electricity generation.12 The produced photocurrent or photovoltage will be highly sensitive to the intensity of incident light. Interactions between the target analyte and the photoelectrode surface can alter PEC reactions, and this can be used for light-controlled sensing or detection based on analyte-induced changes in the photo-response. Bio-photoelectrochemical cells (BPECs) are specialized systems consisting of both bioelectrocatalytic and photoelectrocatalytic components for converting light and chemical energy into electricity simultaneously.13 In addition, BPECs hold the advantages of biocompatibility of EBFCs and robustness of PECs.14
In both BFC- and PEC-based SPECSs, the analyte interaction is linked to the core energy generation mechanism, and the sensing information can be extracted by monitoring the output power of the devices with relatively simple instrumentation. Hence, the processes at the transducer stage can be designed to integrate both the power production and sensing elements closely together to simplify the manufacturing process. Fig. 1 shows the illustration of enzymatic biofuel cells (EBFCs), microbial fuel cells (MFCs) and bio-photoelectrochemical fuel cells (BPFCs).
For the successful realization of BFC- and PEC-based SPECSs, it is essential to consider the use of advanced materials with the capability for rapid electron transfer towards the sensor signal readout. In addition, these advanced materials can support both energy conversion and sensing processes through analyte recognition/interaction mechanisms. Various traditional materials like noble metals,15 carbon nanotubes,16 graphene,17 and conducting polymers18 have been explored for achieving optimal synergy between power generation and sensing performance. However, the stability and biocompatibility of these materials remain significant challenges, which introduce the necessity for novel materials with unique attributes.19
Among the emerging candidates, MXenes, a new family of two-dimensional (2D) transition metal carbides, nitrides, and carbonitrides with unique properties, have garnered substantial interest for electrochemical applications including self-powered sensing applications.20 MXenes are synthesized from their precursor MAX phases via selective etching with hydrofluoric acid or alternative etchants. MXenes possess a characteristic combination of unique properties that make them exceptional candidates for developing integrated sensing and power generation platforms.21 MXenes are represented by the general formula Mn+1XnTx (where M is an early transition metal like Ti, V, Mo, etc.; X is C or N; n = 1–4; and Tx denotes surface functional groups like –F, –O, and –OH).22 They also exhibit excellent metallic conductivity, which ensures efficient charge transport comparable to or exceeding other traditional electrode materials for electrochemical applications in terms of minimizing internal resistance and maximizing power output.23 Also, the field of MXenes has been moving towards employing more environmentally friendly chemicals and methods for their synthesis. The application of diluted fluoride-based etchants,24 electrochemical etching,25 vapour deposition-based synthetic techniques,26 and use of waste streams as precursors will help towards making the MXene a sustainable option.27
Additionally, the surface functionalization of MXenes renders them hydrophilic and provides numerous anchor points for immobilizing enzymes, aptamers, antibodies, or other biorecognition elements, which are essential for highly selective sensing in BFCs.28 Furthermore, the high specific surface area possessed by these materials enables high catalyst loading, thus enhancing the interaction with the surrounding medium (e.g., electrolyte or biological fluid). Some MXenes also exhibit intrinsic electrocatalytic or co-catalytic activity that can be used to replace other expensive catalysts or enhance efficiency in photoelectrochemical systems.29 The tunable surface chemistry along with the possibility of diverse elemental compositions and their ability to form advanced hybrid nanocomposites with other materials open new avenues for modifying their electrocatalytic activity towards specific reactions for energy generation involved in BFCs (like oxygen reduction or fuel oxidation) or PECs.30 The tunable surface chemistry and the presence of hydrophilic groups on MXenes also make these materials friendly for large scale manufacturing because these materials have the ability to be formulated into inks. Formulations of MXenes with biomaterials like enzymes, microbes, and photosynthetic organelles offer attractive opportunities for manufacturing of SPECs.31,32
Xu et al. employed density functional theory (DFT) to unravel the interfacial electronic structure and energetics of MXene/transition-metal oxide (TMO) heterostructures, using –OH, –O–, –F, and mixed-terminated Tin+1CnTx MXenes coupled with anatase TiO2.33 Their results reveal that the magnitude of interfacial charge transfer is highly dependent on MXene surface chemistry. Among the various terminations, OH-functionalized MXenes exhibited the largest work-function disparity (∼1.6 eV for MXene versus 6.4 eV for TiO2), driving substantial electron migration (∼0.9 e nm−2) from the MXene layer into the TiO2 interface. This strong charge redistribution not only lowers the interfacial electronic barrier but also enhances adhesion through hydrogen bonding, thereby establishing an electronically coupled and structurally robust junction. Conversely, O- or F-terminated MXenes exhibited minimal charge transfer and weaker interfacial binding, underscoring the critical role of surface terminations in governing interfacial electronic communication.
While MXene–TMO heterostructures primarily leverage interfacial electron transfer through strong work-function disparities and surface chemistry-driven adhesion, MXene/N-doped graphene hybrids offer a complementary pathway to enhance interfacial kinetics by integrating a highly conductive 2D carbon framework. MXene/N-doped graphene heterostructures exhibit remarkable electrocatalytic efficiency arising from their strong interfacial coupling and accelerated charge-transfer pathways. The DFT calculations also reveal that metallic conductivity of MXenes, combined with the defect-rich, heteroatom-doped graphene network, establishes a seamless electronic interface that minimizes contact resistance and enhances interfacial electron mobility. Nitrogen dopants in graphene introduce localized electronic states near the Fermi level, which act as additional charge reservoirs and facilitate efficient electron tunneling across the heterojunction. Charge density difference maps further confirm pronounced interfacial electron redistribution, indicating strong electronic coupling between MXene and N-doped graphene. This interfacial polarization not only aligns the energy levels between the two components but also optimizes the adsorption energetics of electroactive species, thereby reducing the kinetic barriers for redox reactions. Collectively, the DFT-derived insights highlight how the synergistic interplay of electronic coupling, defect engineering, and interfacial charge polarization in MXene/N-doped graphene heterostructures provides a robust platform for fast electron-transfer kinetics and stable performance in self-powered electrochemical sensors.34
In addition, MXene–polymer interfaces provide another promising strategy to improve the charge-transfer efficiency and interfacial kinetics in SPECSs. As reported using DFT calculations, Ti3C2Tx MXene coupled with polyaniline (PANI) demonstrate pronounced interfacial charge redistribution, with electrons transferring from PANI to MXene due to a favorable Fermi-level alignment. This electron transfer generates an intrinsic interfacial electric field, which facilitates the directional charge flow and significantly reduces the charge-transfer resistance. Partial density of states (PDOS) analysis further reveals the formation of hybridized electronic states at the interface, which act as efficient charge-transport channels. Additionally, this interfacial coupling enhances the adsorption energetics of electroactive species, thereby accelerating redox kinetics crucial for self-powered signal transduction. Looking forward, the rational design of MXene–polymer interfaces, guided by DFT-driven insights, will be critical to overcoming persistent challenges such as interfacial instability, energy loss, and limited operational lifetime, thereby enabling the next generation of highly efficient, durable, and autonomous SPECS platforms.35
These inherent advantages of MXenes, which can overcome the limitations of conventional materials in terms of sensitivity, stability, and miniaturization can be utilized in developing powerful building blocks for next-generation, high-performance SPECSs. Indeed, many conventional materials struggle with insufficient signal response to low analyte concentrations (sensitivity), tend to degrade or lose accuracy over extended use or under harsh conditions (stability), and present considerable fabrication challenges for creating compact, portable devices (miniaturization). The following sections in the review explore how these unique properties of MXenes are utilized in the design and fabrication of MXene-based SPECSs. To provide a clear understanding, the review will specifically discuss systems where MXenes serve as active components, including a detailed comparison of key performance characteristics—such as sensitivity, stability, and operational range—when integrated into EBFC-based, MFC-based, and BPEC-based sensors.
Even though SPECs show great potential, they are often limited in practical applications due to low energy conversion efficiency and limited selectivity, especially in complex samples. As an approach to mitigate these limitations, Sun et al. reported a novel self-powered biosensor employing EBFCs, specifically for ultrasensitive CD44 detection.37 CD44 is a cell-surface molecule involved in many cellular processes and acts as a key biomarker and therapeutic target, especially in cancer metastasis. Hence, the sensitive and specific detection of CD44 is highly essential for diagnostic applications which require advanced sensor platforms. They have synthesized an MXene–AuNP composite, as shown in Fig. 2(a). The developed biosensor consisted of a Au–MXene modified bioanode conjugated with glucose oxidase (GOD) and an aptamer and a bilirubin oxidase (BOx) conjugated Au–MXene modified biocathode, as shown in Fig. 2(b). Initially, the aptamer with high insulation on the bioanode hindered the electron transfer and produced a low open circuit voltage (OCV). When the target CD44 protein was captured by the aptamer at the bioanode, it produced structural changes at the electrode surface, which led to the transfer of electrons and increased the OCV in proportion to the analyte concentration. This clever sensor design achieved a promising LOD of 0.052 ng mL−1, excellent selectivity and stability, proving effective for sensing in real blood samples without any special pre-treatment and highlighting its potential for early cancer diagnosis.
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| Fig. 2 (a) Schematics showing the synthesis of a Au–MXene composite; (b) the schematic illustration of fabrication of the EBFC self-powered sensor with a bioanode and a biocathode and changes in the OCV upon binding with the CD44 protein and the immobilized aptamer. Reproduced with permission from ref. 37, copyright© 2024 Elsevier B.V. | ||
Ji et al. developed a novel enzyme-free intra-capacitive biofuel cell (ICBFC)-based self-powered sensor for the electrochemical detection of endocrine-disrupting phthalates like di(2-ethylhexyl)phthalate (DEHP).38 The sensor design included the integration of a ternary heterostructure capacitive anode and a sensing-interface cathode within a single chamber. The anode was made of Ti3C2Tx MXene, ultra-small AuNPs, and polypyrrole (PPy) NPs in which AuNPs enabled efficient enzyme-free glucose oxidation, while the synergistic combination of MXene's double-layer capacitance and pseudocapacitance of PPy enhanced the charge storage. This sophisticated ICBFC-based self-powered sensor demonstrated a promising LOD of 9.51 pg L−1 for DEHP over a wide linear range, highlighting its potential for rapid, on-site environmental monitoring and public health protection.
In another recent work, Xiao et al. reported a flexible, self-powered biosensor for lactate detection based on carbon cloth electrodes immobilized with lactate oxidase (LOx) and BOx on reduced graphene oxide (rGO).39 Here, MXene was incorporated into a polypyrrole/polyurethane hydrogel and used as a substrate for sensor assembly for placing the electrodes. This integration of MXene hydrogel enhanced the current output by 15-fold due to improved electron mobility and ionic conductivity of MXenes. The developed sensor produced a maximum power density of ∼3 µW cm−2 at 100 mM lactate and showed a linear current response in the physiological window of lactate. This can be used as a biocompatible and scalable route for future wearable applications, enabling accurate, continuous, and self-powered sensing of lactate in physiological environments.
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| Fig. 3 Schematic illustration of the mechanism of self-powered photocatalytic fuel cell (PFC)-based sensors using a Ti3C2Tx MXene–TiO2 composite as the photoanode and Prussian blue (PB) as the cathode for the detection of ochratoxin A. Reprinted with permission from ref. 40. Copyright© 2023, published by Elsevier B.V. | ||
In another work, Jin et al. reported a novel self-powered biosensor by uniquely integrating a photocatalytic fuel cell with a molecular imprinting polymer (MIP) for the detection of aflatoxin B1, which is a highly potent carcinogenic mycotoxin.41 Here, the issue of energy conversion efficiency is tackled by using a MoS2–Ti3C2Tx MXene heterojunction on indium tin oxide (ITO) as a photoanode within the photocatalytic fuel cell which can harness light energy more effectively. The cathode was made by a combination of hemin and graphene to catalyze the reduction of hydrogen peroxide, as shown in Fig. 4. Simultaneously, the selectivity issue is directly addressed by incorporating the MIP, which is designed to specifically capture the target analyte aflatoxin B1 (AFB1) even in the presence of interfering agents. In the absence of AFB1, the photogenerated holes of photoanodes could promote the oxidation of ascorbic acid (AA) and produces an OCV. When AFB1 binds to the cavities of MIP, it affects the OCV of the system, and this change can be used for the specific and sensitive detection of AFB1 with an LOD of 0.73 pg mL−1, as illustrated in Fig. 4. The developed sensor uses this dual approach of MIP for specific target recognition and MXene for efficient light-driven signal conversion for the photocatalytic fuel cell.
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| Fig. 4 Schematics showing the self-powered photocatalytic fuel cell-based biosensor for AFB1 detection. The synthesis of the MoS2–Ti3C2Tx MXene heterojunction and the fabrication of photoanode are given. (a) The conversion of AA into products in the absence of AFB1 produces an OCV and (b) the OCV reduces in the presence of AFB1 as the conversion of AA is blocked. Reprinted with permission from ref. 41. Copyright© 2021, American Chemical Society. | ||
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| Fig. 5 The schematic showing the fabrication of a dual-power-peak photofuel cell (PFC)-based self-powered sensor for the detection of chloramphenicol. (a) Fabrication of the photoanode. (b) Fabrication of the photocathode. (c) Construction of the dual-power-peak PSPS combining the photoanode and photocathode. (d) Schematic illustration showing the dual-power-peak detection configuration in the presence of K2S2O8. Reprinted with permission from ref. 43. Copyright© 2023, Elsevier B.V. All rights reserved. | ||
Ultrasensitive detection of potent toxins like microcystin-RR (MC-RR) is highly critical for environmental safety evaluation and need to fabricate advanced portable and real time sensors with efficient signal amplification for sensitive detection. Towards this aspect, Sun et al. constructed a photo-driven self-powered BPEC aptasensor for MC-RR using the Ti3C2Tx/ZnIn2S4 heterojunction as the photoanode and Cu2O as the photocathode.42 The Ti3C2Tx MXene in the system enhances charge separation in addition to providing a large surface area for immobilization of the MC-RR specific aptamer. When MC-RR binds to the aptamer, it causes a ‘signal-off’ mechanism due to steric hindrance, which reduces the photocurrent. In addition, they integrated a matching capacitor, boosting the sensitivity by 22-fold and proposed a USB-sized micro-workstation for capturing instantaneous signals to make the system portable. Under optimal conditions, this multi-amplification system achieved the photocurrent in a linear relation with the concentration of MC-RR with an extremely low LOD of 0.033 pM and demonstrated the practical applicability of the system in fish samples.
In a different approach, a novel dual-power-peak photofuel cell (PFC)-based self-powered sensor has been developed for the detection of chloramphenicol by introducing dual peak output signals for enhancing the detection accuracy.43 They have utilized persulfate as an initiator for getting a dual peak response in the PFC system, which can enhance charge separation and generate a second power peak in the output signal. The photoanode was made of fluorine-doped tin oxide (FTO) modified with BiVO4 and V2C MXene, followed by modification with an aptamer, as seen in Fig. 5(a). The incorporation of V2C MXene accelerates electron transfer, boosting photoelectric conversion efficiency, while the aptamer provides specific recognition of chloramphenicol. FTO modified with molybdate hexacyanoferrate (MoHCF) was used as a photocathode, as shown in Fig. 5(b). The construction of the dual-power-peak photocatalytic fuel cell-based self-powered sensor is given in Fig. 5(c). When chloramphenicol binds to the aptamer on the photoanode, the output signal of the sensor, including two power peaks, changed linearly with the concentrations of chloramphenicol (Fig. 5(d)). The quantification of chloramphenicol based on these dual power peaks allowed sensitive detection with an LOD of 0.17 pM over a linear range of 0.5 pM to 3 nM, demonstrating a promising strategy for developing highly sensitive and specific multi-signal self-powered sensors.
Various other self-powered sensors have been developed by using MXenes as one of their components. In this aspect, Liu et al. developed a novel dual-modal zinc–air battery (ZAB) driven self-powered electrochemical aptasensor based on the heterojunction of V2CTx MXene and bimetallic CoNi-layered double hydroxide (CoNi-MLDH) for the detection of cortisol.46 They utilized V2CTx nanosheets as scaffolds for the in situ growth and subsequent formation of CoNi-MLDH nanosheets. The V2CTx MXene in the CoNi-MLDH composite enhances the electrochemical activity, while the CoNi-LDH enhances the surface area, functionality, oxygen reduction activity, and aptamer affinity of the composite. By utilizing these advantages, the developed ZAB driven self-powered aptasensor was able to achieve a very low LOD of 0.17 fg mL−1 for cortisol.
In another work, a similar ZAB-based self-powered aptasensor was proposed by Liu et al. for the detection of penicillin G by using a Zn plate photoanode and a heterojunction made of cadmium-doped MoS2 nanosheets grown on Ti3C2Tx MXene (Cd–MoS2@Ti3C2Tx) as the photocathode.47 Fig. 6 shows the schematics of the fabrication of a photo-assisted ZAB-driven self-powered aptasensor and detection process by binding the aptamer with penicillin G. The enhanced light absorption, high photoelectric conversion efficiency, and more catalytic active sites of this heterojunction boost the ZAB output voltage to 1.43 V under UV-vis light irradiation. The resulting self-powered aptasensor displayed an ultralow LOD of 0.06 fg mL−1 for penicillin G, with promising specificity and stability, offering a promising portable sensor for the detection of antibiotics.
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| Fig. 6 Schematic diagram showing the fabrication steps for the photo-assisted ZAB-driven self-powered aptasensor for the detection of penicillin G and the mechanism of detection of penicillin G. Reprinted with permission from ref. 47. Copyright© 2023, Elsevier B.V. | ||
The path to functional integration of energy harvesters with sensing circuits is also complicated by the variable and pulsed nature of the generated electrical signals. These fluctuations can make accurate signal measurement difficult and may lead to unwanted phenomena at the electrode, such as the build-up of polarization or secondary chemical reactions that are not part of the intended sensing process. When several energy harvesting elements are combined, phase mismatches can occur, leading to irregular signal shapes and increased risk of sensor aging due to surface passivation. While using alternative current generation regimes can sometimes help mitigate these effects, it adds to the complexity of sensor design and the need for precise electrical matching. These SPECSs inherently face the challenge of limited energy conversion efficiency due to constrained power harvesting, inefficient interfacial coupling, and low signal transduction rates.48
Another central challenge lies in the properties and robustness of the electrode materials themselves. While MXene electrodes offer high electrical conductivity and rich surface terminations, practical issues such as restacking of nanosheets and agglomeration significantly reduce the accessible surface area and block redox-active sites, resulting in lower energy output and diminished sensor sensitivity. Even beyond MXenes, non-MXene materials like carbon nanotubes and metal oxides also hit similar efficiency barriers, such as poor wettability, sluggish electron–ion transport, and weak electrode–solution coupling, hampering comprehensive energy-to-signal conversion in autonomous sensing configurations.49
In addition to efficiency, operational instability poses a critical limitation to SPECS lifespan, particularly in wearable or biological environments. MXene materials are prone to oxidation, especially under exposure to humidity or oxidative conditions, leading to conductivity degradation and signal drift over time. Biological deployment further introduces biofouling, molecular adsorption, and environmental interference, all of which can obstruct electrode surfaces and disrupt consistent sensing performance. Similarly, non-MXene systems such as conductive polymers or metal oxide sensors face structural deformation, polymer degradation, or loss of receptor function limitations that shorten device lifetimes and affect repeatability.50
Finally, scalability, reproducibility, and sensor specificity remain formidable obstacles to commercialization. MXene fabrication often depends on harsh etching techniques, leading to variability in surface termination (–O, –OH, and –F), flake size, and defect density—factors that directly affect electrochemical performance and batch-to-batch consistency. On the non-MXene side, heterogeneous hybrids of organic and inorganic elements often struggle with inconsistent receptor attachment, limited analyte specificity, and low selectivity, reducing the accuracy in real-world deployments. Addressing these challenges will require green, standardized manufacturing processes, robust surface chemistries, and integrated receptor design to ensure a reproducible, selective, and commercially viable SPECS platform.48,51
In sum, advancing self-powered electrochemical sensors to practical, widespread use will demand solutions that improve both energy harvesting and material stability while also enabling reliable mass production. Progress toward more sustainable production, better integrated circuit management, and the development of robust, durable interfaces will be key steps. Only by tackling these challenges in concert will the promise of self-powered sensing technologies be fully realized.
A solid foundation for the advancement of SPECs has been laid by several key research efforts. Wang and coworkers were pioneers in the field, establishing the concept of wearable self-powered sensors and on-body power grids.52,53 This work created a crucial framework for integrating energy harvesting with sensing technology. Building on this, Yin et al. demonstrated the use of passive perspiration-based biofuel cells, a concept that can be realized with great efficiency using MXenes due to their high conductivity, hydrophilicity, and ability to preserve the function of power-generating biocomponents.54 This work provides a clear roadmap for harnessing the unique properties of MXenes in practical applications. Furthermore, a critical question regarding the biocompatibility of MXenes for wearable applications was addressed by Gao and coworkers, who successfully developed an MXene-based platform for monitoring female hormones, thereby proving its viability for direct human use.55
Based on the provided data, a direct quantitative comparison between MXene-based SPECSs and conventional materials is challenging due to the early stage of MXene research and diverse device architectures. However, qualitative contrasts can be made in this aspect. MXene-based devices often demonstrate comparable or superior sensitivity and fast response times for specific analytes, as shown by the pM-level detection limits for lead ions and the dynamic ranges for other proteins. For instance, the Au–MXene device for CD44 protein shows versatility with its wide dynamic range. Additionally, MXenes show promising stability with a 98.49% signal retention after 15 days for a cortisol sensor.37 This is a significant finding as stability is often a major challenge for nanomaterial-based devices (Table 1). Table 1 shows a comparative analysis of SPECSs based on MXenes with other nanomaterials. An analysis of Table 1 indicates that MXene- and non-MXene-based SPECSs exhibit similar stability and performance metrics. In addition, MXene-based modifications are expected to possess better aqueous solution processibility than their pristine carbon counterparts, which makes them more environmentally sustainable for use in SPECSs. However, the heterogeneity in reported electrode construction—specifically the varying methodologies, protocols, and modification layers—precludes a comparison of the true stability performance across these reports. A proposed benchmark for MXene-based SPECSs is the attainment of higher stability metrics using smaller form factors.
| Anode | Cathode | Analyte | LOD | Dynamic range | Construction and performance metrics (Pmax/EOCV) at the baseline | Stability | Ref. |
|---|---|---|---|---|---|---|---|
| Two-dimensional lamellar gold nanoparticles–Ti3C2Tx (AuNPs–Ti3C2Tx) heterostructures | Doped carbon-based nanosheets | Lead ion (Pb2+) | 0.43 pM | 0.01–7500 nM | Beaker-based | ∼92% of the initial level after 45 days | 36 |
| Eocv: 367 mV | |||||||
| MXene–AuNP composite modified with glucose oxidase (GOx) and an aptamer | Au–MXene modified with bilirubin oxidase (BOx) | CD44 protein | 0.052 ng mL−1 | 0.5–1000 ng mL−1 | Beaker-based | ∼97% after 15 days | 37 |
| Pmax: ∼1 µW cm−2 | |||||||
| EOCV: 390 mV | |||||||
| Ti3C2Tx MXene, ultra-small AuNPs, and polypyrrole (PPy) NPs (ternary heterostructure capacitive anode) | A sensing-interface cathode within a single chamber | Di(2-ethylhexyl)phthalate (DEHP) | 9.51 pg L−1 | 0.05 to 100 000 ng L−1 |
Beaker-based | 93.2% after 30 days | 38 |
| Anode is non-enzymatic glucose-based, which drives the cathode-based DEHP sensor | |||||||
| Ti3C2Tx MXene–TiO2 composite photoanode | Prussian blue (PB) cathode | Ochratoxin A | 0.0587 ppb | 0.2–20 ppb | Beaker-based | 85.2% of the initial level after 7 days | 40 |
| Pmax: ∼15.015 µW cm−2 | |||||||
| EOCV: ∼440 mV | |||||||
| MoS2–Ti3C2Tx MXene heterojunction on indium tin oxide (ITO) | Hemin and graphene composite | Aflatoxin B1 (AFB1) | 0.73 pg mL−1 | 0.01–1000 ng mL−1 | Beaker-based | 97% of the initial level after 7 days | 41 |
| EOCV: ∼465 mV in PBS, milk, oil, and maize | |||||||
| Ti3C2Tx/ZnIn2S4 heterojunction photoanode | Cu2O photocathode | Microcystin-RR (MC-RR) | 0.033 pM | 0.1 to 100 pM | Portable device | Unchanged after continuous cycling every 7 days | 42 |
| Pmax: ∼26 µW | |||||||
| EOCV: ∼450 mV | |||||||
| BiVO4 and V2C MXene on fluorine-doped tin oxide (FTO) | Molybdate hexacyanoferrate (MoHCF) | Chloramphenicol | 0.17 pM | 0.5 pM to 3 nM | Beaker-based | 97.99% signal after 6 cycles every 2 days | 43 |
| Pmax: 0.626 µW cm−2 under light irradiation | |||||||
| V2CTx MXene and bimetallic CoNi-layered double hydroxide (CoNi-MLDH) heterojunction | Zinc (Zn) plate anode | Cortisol | 0.17 fg mL−1 | 10 fg mL−1 to 100 ng mL−1 | Device based on a glass substrate | 98.49% after 15 days | 46 |
| EOCV: 1130 mV | |||||||
| Zinc (Zn) plate photoanode | Cadmium-doped MoS2 on the Ti3C2Tx MXene (Cd–MoS2@Ti3C2Tx) heterojunction photocathode | Penicillin G | 0.06 fg mL−1 | 1.0 fg mL−1 to 0.1 ng mL−1 | Beaker-based | 96.4% after 20 days | 47 |
| Pmax: ∼2500 µW cm−2 | |||||||
| EOCV: ∼1100 mV | |||||||
| Pencil graphite–MWCNT/pyrroloquinoline quinone-dependent glucose dehydrogenase (PQQGDH) | Pencil graphite–MWCNT/bilirubin oxidase (BOx) | Glucose | 0.084 mM | Up to 1 mM | Beaker-based | 94% after 12 days | 56 |
| Pmax: ∼2.5 µW cm−2 | |||||||
| EOCV: ∼450 mV | |||||||
| Carbon paper (CP)/ultrathin hollow carbon shells (UHCS)/gold nanoparticles (AuNPs)/polydopamine film/laccase | DNA1/UHCS/AuNPs/CP | L-Cysteine | 2.2 nM | 0.01–5 µM | Beaker-based | 97% after 2000 s | 57 |
| EOCV: ∼360 mV | |||||||
| Carbon cloth/AuNPs/graphdiyne/glucose oxidase/bovine serum albumin | Carbon cloth/AuNPs/graphdiyne/AuNPs/T-DNA/MCH/DNA nanorods | miRNA-141 | 21.9 aM | 0.0001 to 100 pM | Beaker-based | 96.0–97.3% after 12 days | 58 |
| EOCV: ∼175 mV | |||||||
| Crystalline polymeric carbon nitride/SWCNT film | SWCNT/Pt NPs | Peroxide | 0.006 mM | 0–1.0 mM | Microfluidic-based | Unchanged for 7 days | 59 |
| Photoelectrochemical sensing mechanism regulated by electrocatalytic current |
The current lab-scale, beaker-based nature of these devices suggests a low Technology Readiness Level (TRL), likely TRL 1 to TRL 4. This means the primary focus is on establishing fundamental principles and feasibility in a controlled environment. Real-world performance under various environmental conditions like humidity and temperature is typically assessed at higher TRLs (e.g., TRL 5 and 6). Therefore, further research is necessary to move these technologies from the lab to a fabricated device that can be systematically tested under real-world conditions to address these concern and evaluate its resilience to environmental stressors.
The degree of hydrophilicity observed in these materials was found to depend heavily on both etching media, whether it is a single acid like HF or a combination of acids such as H2SO4 and HF or HCl and HF. Interestingly, Ti3C2Tx exhibited a greater retention of structural water when fewer oxygen-based terminations were present on the surface. Furthermore, employing milder etching conditions or mixed acid systems led to improved thermal robustness by minimizing defect sites during synthesis. The thermal durability of MXenes is closely linked to their intrinsic structure and elemental makeup. Among them, Ti3C2Tx exhibits superior heat resistance compared to Mo2CTx and Nb2CTx, both of which possess fewer atomic layers. Between the latter two, Mo2CTx is thermally more robust than Nb2CTx.61
Numerous research ideas have highlighted that the structural integrity of MXenes is governed by a combination of external chemical conditions and inherent material properties, such as atmospheric exposure, temperature, compositional variations, microstructural features, and interactions with aqueous environments. Furthermore, even MXenes sharing the same chemical composition can display markedly different oxidation behaviours, primarily due to variations in their synthesis techniques and processing conditions.
Extensive investigations have been carried out to understand the thermal and chemical stability of MXenes under different atmospheric conditions such as vacuum, inert, oxidizing, and reducing environments. For instance, Ti3C2 MXenes have been reported to remain structurally stable in an argon atmosphere even at elevated temperatures of up to 800 °C. In contrast, when subjected to oxygen-rich conditions, oxidation begins at relatively low temperatures (200 °C), leading to the uniform formation of anatase across the surface. Upon heating to 1000 °C, this anatase phase further transforms completely into rutile.63,64 A detailed evaluation of V2CTx MXenes was carried out by Thakur et al., who examined their stability in air, CO2, H2, and N2 atmospheres at temperatures of up to 600 °C. They reported that above 300 °C, V2CTx readily oxidized in air or CO2, producing V2O5 and other VOx phases, along with a complete collapse of the layered architecture. Under a reducing H2 atmosphere, however, partial retention of the layered structure was observed. Exposure to N2 led to mild oxidation, attributed to trace H2O molecules incorporated during the synthesis process, which reacted with the surface groups of V2CTx.65
The oxidation of MXenes occurs more rapidly when they are dispersed in aqueous media compared to their freestanding form. Earlier studies attributed this instability mainly to dissolved O2 in water. However, more recent evidence suggests that MXenes are inherently more reactive toward H2O molecules than toward dissolved oxygen.66 Beyond neutral solutions, investigations have been extended to alkaline and oxidizing environments. Doo et al. demonstrated that pH plays a critical role in dictating the oxidation pathway of aqueous Ti3C2 dispersions. They proposed a distinct mechanism in which the terminal –OH groups interact with either H+ or OH− ions, generating different reaction intermediates depending on the pH.67 Complementing this, Zhao et al. showed that alkaline conditions accelerate MXene oxidation, where hydroxyl ions significantly enhance the conversion of Ti species. This conclusion was supported by X-ray photoelectron spectroscopy (XPS) analysis, which revealed an increased proportion of Ti(IV) species in basic media.68 The stability and performance of MXenes depend on multiple factors, including the method of synthesis, the nature of surface terminations, structural stability, and particle size, all of which need to be carefully optimized to ensure their effective use in a wide range of applications.
Oxidation in MXenes is often initiated at reactive surface terminations, particularly hydroxyl groups, which are highly vulnerable to oxidative attack. One approach to suppress this process involves the removal of surface terminations through thermal annealing under vacuum or inert environments. Such treatments enhance the inherent thermal stability of MXenes and extend their applicability in high-temperature settings. For instance, Wang et al. demonstrated that MXenes stripped of surface terminations could withstand heating up to 1200 °C under an argon atmosphere.69 Similarly, Zhao et al. reported that annealing Ti3C2Tx in argon promoted the formation of a thin, protective TiO2 layer on the nanosheet surface. This oxide barrier, particularly effective in densely stacked films, restricted water penetration and preserved the internal structure. Compared to untreated Ti3C2Tx, the annealed films exhibited remarkable stability, maintaining their structure for over ten months in aqueous environments, thereby significantly expanding their potential in practical applications.70
In addition to thermal treatments, storage protocols play a crucial role in maintaining the integrity of MXenes. Studies have shown that both the temperature and atmospheric composition directly affect their chemical stability. Zhang et al. recommended extending the lifetime of MXene dispersions by storing concentrated nanosheet suspensions with large lateral sizes in sealed, argon-filled containers at low temperatures.71 Other studies further highlighted that excluding dioxygen and refrigerating dispersions help to minimize oxidative degradation. The solvent medium also influences stability: Maleski et al. compared Ti3C2Tx dispersions in 12 different solvents and found that polar organic solvents such as N,N-dimethylformamide (DMF), N-methyl-2-pyrrolidone (NMP), and propylene carbonate (PC), and ethanol significantly reduced oxidation compared to water. Similarly, isolation of MXene powders from aqueous suspensions via freeze-drying or vacuum filtration was reported as an effective approach to prevent aqueous-induced degradation. Collectively, these strategies demonstrate that careful optimization of storage conditions is essential for prolonging the MXene lifetime in both solution and solid states.72
Chemical modification and antioxidant incorporation represent another major pathway for enhancing MXene stability. Analogous to food preservation methods, antioxidants such as sodium L-ascorbate (NaAsc) have been employed to protect MXene dispersions. Zhao et al. showed that NaAsc forms a stabilizing layer around Ti3C2Tx nanosheets, effectively inhibiting oxidation and maintaining their structure and conductivity for up to three weeks at room temperature.73 Similarly, Natu et al. demonstrated that adding polyanionic salts (polyphosphates, polyborates, and polysilicates) at low concentrations can suppress oxidation initiated at nanosheet edges by creating a protective electrostatic barrier.74 Beyond antioxidants, functionalization with silanes,75 polymer coatings76 and biomolecules such as silk fibroin77 has been shown to improve hydrophobicity, enhance interfacial interactions, and provide protective encapsulation against oxidative attack. Furthermore, nanoscale carbon coatings offer an effective route to stabilize MXenes during synthesis. Overall, surface functionalization strategies including antioxidants, polymers, proteins, and carbon coatings provide versatile and effective means to suppress oxidation while retaining the functional properties of MXenes, thereby extending their performance in electrochemical and other applications.
On combining these approaches, process enhancement, solvent choice, antioxidant addition, thermal passivation and encapsulation dramatically extend the lifespan of MXene materials and help retain their electronic and structural properties. These advances pave the way for integration of MXenes into real-world SPECS devices, enabling high efficiency, durable self-powered sensing in applications ranging from environmental monitoring to wearable diagnostics.
The future trajectory for MXene-based SPECSs is exceptionally bright, contingent upon addressing the current limitations. The challenges of long-term operational stability and degradation (Section 5) can be overcome by focusing future research on precise surface engineering and the rational design of novel heterostructures (Section 7). To combat the issue of reproducible, scalable, and cost-effective synthesis (Section 5), future efforts should be directed toward scalable micro-/nanofabrication techniques for device miniaturization (Section 7). Furthermore, the limited understanding of charge transfer mechanisms and the integration of multiple components into miniaturized, robust devices (Section 5) necessitate a deeper fundamental investigation into these systems to unlock the full potential of MXenes for creating transformative autonomous sensing devices. By explicitly addressing these limitations through concerted research and development efforts, the field can transition from laboratory successes to impactful real-world applications.
Towards improving energy conversion efficiencies, MXene integrated energy storage systems with better power management and exploring hybrid energy harvesting modes along with advancing scalable micro-/nanofabrication techniques for device miniaturization need to be considered. For rational design optimization of MXene-based systems, a deeper fundamental understanding of charge transfer mechanisms and synergistic effects in complex MXene-based systems should be thoroughly investigated. Moreover, the effective energy management solutions should be applied for certain high-demand applications, and the significant engineering challenges in the integration of multiple components into miniaturized, robust devices need to be solved.
Further exploration could involve MFCs, which have been realized using diverse electrode materials and are being considered for wearable and environmental sensing.78–81 Given that MXenes have already demonstrated success in MFC device realization, attributable to their high electrical conductivity, large active surface area, inherent biocompatibility, and ability to facilitate efficient extracellular electron transfer (EET), the focused application of MXene-based MFCs for self-powered wearable and environmental sensing presents a compelling, yet relatively underexplored, research avenue.82–84 Future reports could specifically address this niche, bridging the gap in leveraging these advanced MXene–MFC systems for such targeted sensing applications. Similarly, a parallel research thrust could explore applications of MXenes in self-powered devices integrating photosynthetic systems. This could involve employing isolated photosynthetic receptors (like thylakoids),85 or whole microorganisms,86 such as algae,87 phytoplankton,88 and potentially engineered yeast strains, thereby opening further avenues for novel bio-hybrid sensor development—an area also warranting deeper future investigation, including the potential role of MXenes in enhancing such photosynthetic bio-interfaces.
Nevertheless, the future trajectory for MXene-based SPECSs is exceptionally bright for translating laboratory successes into impactful real-world applications. By addressing the current limitations through these concerted research and development efforts, the field of MXene-based SPECSs can unlock the full potential of MXenes to create truly transformative autonomous sensing devises for diverse applications.
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