Open Access Article
Enas Daouda,
Bakr Imad Najmb,
Omayma Salim Waleedc,
Maharshikumar B. Shuklad,
Rekha M. M.e,
Y. Sasikumarf,
Vipasha Sharmag,
Ahmed Aldulaimih and
Sharmin Smaeilpour
*i
aFaculty of Allied Medical Sciences, Hourani Center for Applied Scientific Research, Al-Ahliyya Amman University, Amman, Jordan
bCollege of Pharmacy, Department of Pharmaceutical Sciences, AL-Turath University, Baghdad, Iraq
cDepartment of Anesthesia Techniques, Health and Medical Techniques College, Alnoor University, Mosul, Iraq
dDepartment of Chemistry, Faculty of Science, Gokul Global University, Sidhpur, Gujarat, India
eDepartment of Chemistry and Biochemistry, School of Sciences, JAIN (Deemed-to-be University), Bangalore, Karnataka, India
fDepartment of Chemistry, Sathyabama Institute of Science and Technology, Chennai, Tamil Nadu, India
gDepartment of Biotechnology, University Institute of Biotechnology, Chandigarh University, Mohali, Punjab, India
hFaculty of Pharmacy, Al-Zahrawi University, Karbala, Iraq
iYoung Researchers and Elite Club, Islamic Azad University, Tehran Branch, Tehran, Iran. E-mail: sharminsmaeilpour@gmail.com
First published on 4th June 2026
Heteroatom-doped MXene quantum dots (MQDs) have emerged as promising fluorescent nanoplatforms for the selective detection of transition metal ions such as Fe3+, Cu2+, Zn2+, and Mn2+. Their tunable electronic structure, high quantum yield, and versatile surface chemistry enable precise modulation of optical properties and binding interactions with metal ions. This review provides a comprehensive overview of recent advances in the design and application of heteroatom-doped MQDs for transition metal ion sensing. Particular emphasis is placed on atomic-level engineering strategies, including dopant–host electronic coupling, defect–dopant synergy, single-atom doping, selective functionalization at edge versus basal-plane sites, and multi-element doping (e.g., S, P, B, and halogens). These structural modifications enable tailored control over charge distribution, redox activity, and coordination environments, thereby improving sensitivity and ion selectivity. Beyond conventional fluorescence quenching mechanisms, emerging sensing strategies are also discussed, including ratiometric detection, stimuli-responsive probes, multimodal sensing systems integrating optical, electrochemical, and visual signals, and logic-gated or data-assisted sensing approaches designed to improve analytical reliability in complex matrices. Representative sensing behaviors are highlighted, such as redox-mediated quenching for Fe3+ and Cu2+, fluorescence enhancement for Zn2+, and dual-emission ratiometric recognition for Mn2+. Finally, current challenges—including synthesis scalability, selectivity in competitive environments, matrix interference, and translation toward deployable sensing devices—are critically evaluated, and future directions for portable sensing platforms and intelligent analytical systems are discussed.
In this landscape, MXene quantum dots (MQDs)—ultrasmall, zero-dimensional derivatives of two-dimensional MXenes—have garnered substantial attention as next-generation fluorescent nanomaterials.18,19 MXenes, a family of transition metal carbides, nitrides, or carbonitrides with the general formula M{n+1}XnTx (where M is a transition metal, X is carbon/nitrogen, and Tx denotes surface terminations), exhibit exceptional properties including high electrical conductivity, hydrophilic surfaces, and tunable bandgaps. When downsized to quantum dots via exfoliation or bottom-up synthesis, MQDs inherit these attributes while gaining quantum confinement effects, leading to bright photoluminescence (PL), high quantum yields (QYs), and excellent photostability. Unlike traditional QDs (e.g., CdSe or InP), MQDs are composed of earth-abundant elements, offering biocompatibility and reduced toxicity, making them suitable for bioenvironmental applications.20–22 The rich surface chemistry of MQDs, characterized by abundant functional groups (–OH, –O, –F), enables facile modification for targeted sensing.
It is important to distinguish MQDs from their bulk or two-dimensional MXene counterparts. While bulk MXenes primarily exhibit metallic conductivity and layered structures with relatively uniform electronic behavior, MQDs possess ultrasmall dimensions typically below 10 nm. At this scale, strong quantum confinement and a high density of edge and defect sites significantly modify their electronic structure, surface chemistry, and photoluminescence properties. These size-dependent effects generate discrete energy states and enhanced surface reactivity, which are key factors enabling MQDs to function as highly sensitive platforms for fluorescence-based ion sensing.
Heteroatom doping represents a transformative strategy to enhance the sensing capabilities of MQDs. By incorporating non-metal elements such as nitrogen (N), sulfur (S), phosphorus (P), boron (B), or halogens into the MQD lattice, researchers can precisely modulate electronic structure, charge distribution, and surface reactivity.23,24 This atomic-level engineering shifts MQDs from passive emitters to active recognition platforms. For instance, N-doping introduces electron-donating states, enhancing PL efficiency and creating coordination sites for metal ions, while S-doping imparts redox-active properties for selective quenching. Co-doping (e.g., N + S) synergistically amplifies these effects, enabling emergent behaviors like ratiometric responses.23,25 Such modifications address key challenges in transition metal ion sensing: achieving nanomolar sensitivities, discriminating between ions with similar redox potentials, and maintaining robustness in interferent-rich matrices.
The evolution of MQD-based sensors has progressed from basic intensity-based quenching to sophisticated paradigms. Early designs focused on static fluorescence modulation, where ion coordination disrupts radiative recombination, leading to “turn-off” signals. However, these are susceptible to environmental artifacts. Recent advancements emphasize ratiometric architectures, where dual-emission channels provide self-calibration, mitigating fluctuations in probe concentration or excitation intensity. Stimuli-responsive systems further introduce adaptability, allowing reversible “on–off” cycles in response to pH or competing analytes.27,28 Multimodal integration—combining optical, electrochemical, and visual outputs—enhances versatility, while logic-gated and sequential recognition encode chemical events as computational operations, suppressing false positives in multi-ion environments. Data-integrated platforms, leveraging machine learning for pattern analysis, foreshadow intelligent sensing ecosystems.29,30
Performance analyses underscore the efficacy of heteroatom-doped MQDs for specific ions. For redox-active Fe3+ and Cu2+, amino-functionalized Ti3C2 MQDs achieve quenching-based detection with limits of detection (LODs) in the low nanomolar range, suitable for environmental thresholds. Zn2+ sensing exploits “turn-on” enhancement via excited-state stabilization, offering selectivity over quenching-prone ions. Mn2+ detection benefits from dual-emission ratiometry, providing robust quantification in mineral waters. Emerging Nb2C-based MQDs expand material diversity, combining sensing with bioimaging.31–33 Selectivity engineering, via masking agents or differential signal patterns, addresses competitive binding, while portability trends—test strips and smartphone readers—facilitate field deployment.
Despite these strides, challenges persist. Synthesis scalability remains limited by batch variability and high-energy processes, hindering commercial viability. Fundamental selectivity boundaries arise from overlapping ion affinities, necessitating computational-guided design. Matrix robustness under variable conditions (e.g., pH, salinity) demands further optimization. Future directions include IoT integration for continuous monitoring, biocompatible formulations for in vivo sensing, and multifunctional devices for simultaneous multi-ion analysis.26–28
This review examines heteroatom-doped MQDs as promising platforms for selective transition metal ion sensing. It integrates atomic-level design strategies—dopant–host coupling, defect synergy, single-atom precision, spatial doping control, and multi-element expansion—with advanced recognition paradigms, including ratiometric, stimuli-responsive, multimodal, logic-gated, sequential, and intelligent data-driven systems. Ion-specific performance for Fe3+, Cu2+, Zn2+, and Mn2+ is assessed, alongside selectivity enhancement in complex matrices and pathways to portable, deployable formats. Key challenges in scalability, matrix robustness, selectivity limits, and integration are evaluated, while future directions such as computational optimization, IoT networks, and bioanalytical multifunctionality are outlined. This work synthesizes recent high-impact progress to guide the evolution of MQD-based technologies in environmental monitoring, water quality, food safety, and biomedical applications. This review primarily focuses on advances in MXene quantum dots reported during the period 2021–2026, highlighting the most recent developments in heteroatom doping strategies and sensing applications, while selectively citing earlier studies to provide essential background for the field.
Several recent reviews and studies have examined MQDs from different perspectives. Previous works have mainly focused on multifunctional water remediation combining photocatalysis, electrocatalysis, and fluorescence sensing,33 as well as nitrogen-doped MQDs emphasizing mechanistic fluorescence, electrochemical, and electrochemiluminescence sensing platforms.19,27 Other studies have investigated engineered MQDs for energy-related applications such as micro-supercapacitors rather than selective sensing.29 In contrast, the present review provides a broader design-oriented framework that systematically correlates heteroatom doping beyond nitrogen, atomic-level structural engineering, and advanced recognition paradigms—including ratiometric, multimodal, and logic-gated sensing—specifically for selective transition metal ion detection. This integrated structure–mechanism–performance perspective distinguishes the scope of this review.
From a materials design perspective, the electronic role of dopants is governed by their electronegativity, valence configuration, and coordination preferences relative to the parent MXene lattice. Substitutional dopants can introduce localized donor or acceptor states, while interstitial or surface-anchored dopants may act as charge polarization centers. These effects lead to spatially heterogeneous electronic landscapes within a single MQD, creating regions with distinct redox potentials and electron affinity. Such heterogeneity is particularly relevant for transition-metal ion interactions, as it dictates preferential adsorption and coordination sites at the nanoscale.36
Importantly, dopant–host coupling in MQDs is strongly size-dependent. As MQD dimensions approach the exciton Bohr radius, even low dopant concentrations can dominate electronic behavior. This sensitivity necessitates precise control over dopant placement and concentration, shifting the design paradigm from average composition toward atomistic precision. Emerging synthetic approaches increasingly aim to regulate dopant-induced electronic anisotropy, enabling rational control over MQD reactivity without relying on post-synthetic functionalization.37,38 This atomic-level understanding forms the foundation for next-generation MQD design strategies.
Panels (1a) and (1d) provide clear spectroscopic evidence that nitrogen incorporation modifies the electronic interaction between dopant atoms and the Ti2C host lattice. The XPS survey spectrum (Fig. 1a) shows a decrease in oxygen-related signals together with stronger Ti and C contributions, indicating that the Ti2C framework remains largely preserved during the doping process. This observation suggests that nitrogen incorporation occurs without extensive oxidation of the MXene structure. The Ti 2p spectrum (Fig. 1d) further supports this interpretation, where the dominant Ti–C peaks confirm the integrity of the Ti–C lattice, while only weak Ti–O features are observed. The preservation of Ti–C bonding together with the presence of nitrogen indicates that dopants interact electronically with the Ti2C lattice rather than forming separate oxide phases. Consequently, nitrogen atoms introduce new electronic states within the MQD structure, modifying the local charge distribution and strengthening dopant–host electronic coupling within the quantum-confined lattice.
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| Fig. 1 (a) XPS survey spectrum, (b) high-resolution C 1s, (c) O 1s, (d) Ti 2p, (e) N 1s, and (f) FT-IR spectra of N-Ti2C MQDs, revealing dopant–host electronic coupling and defect-stabilization effects through preservation of Ti–C bonding and nitrogen-induced localized electronic states. This figure has been reproduced from ref. 38 with permission from American Chemical Society, copyright 2021. | ||
Atomic vacancies, particularly metal or carbon vacancies, can act as anchoring centers for heteroatoms, lowering the formation energy of doped structures. When a dopant occupies a vacancy-adjacent site, local coordination symmetry is disrupted, leading to asymmetric charge redistribution. This asymmetry can induce localized dipole moments and strain fields, both of which strongly influence surface chemistry.41–43 Such coupled defect–dopant motifs often exhibit electronic states within the bandgap, enabling fine control over charge transfer processes.
Edge defects play an even more prominent role in MQDs due to their high proportion relative to basal planes. Edge-selective doping strategies exploit the undercoordinated nature of edge atoms to introduce heteroatoms with minimal lattice disruption. The resulting edge-confined active sites combine structural flexibility with electronic tunability, offering a versatile platform for controlled interactions with external species.40,44 From a design standpoint, the deliberate coupling of defects and dopants represents a shift from defect minimization toward defect utilization, enabling the creation of function-specific MQDs with tailored atomic architectures.
Fig. 1b and c provide insight into how dopants interact with defect-rich regions formed during quantum dot generation. The reduced intensity of C–O components in the C 1s spectrum (Fig. 1b), together with the simplified O 1s profile dominated by Ti–O and C–Ti–(OH)x bonds (Fig. 1c), indicates that defect-induced oxidation pathways are effectively suppressed. Given the high density of undercoordinated sites created as Ti2C MXenes are converted into MQDs, these observations suggest preferential dopant interaction with defect-adjacent sites, stabilizing them against further structural degradation.
The FT-IR spectrum in Fig. 1f, in conjunction with the N 1s spectrum (Fig. 1e), further supports the formation of coupled defect–dopant motifs. Vibrational signatures associated with C–N and N–H groups indicate that nitrogen-containing functionalities are selectively anchored at defect-prone surface regions. Rather than acting as passive surface terminations, these dopant-modified sites actively reshape the defect landscape, converting intrinsically reactive imperfections into electronically stabilized motifs. This behavior exemplifies defect utilization rather than defect elimination.
Fig. 2 illustrates the synthetic pathway leading to the formation of N-doped MQDs from Ti3AlC2 MAX precursors and provides mechanistic insight into how defect–dopant coupling emerges during the process. The LiF/HCl etching step selectively removes Al layers, producing Ti3C2 MXene sheets rich in surface terminations and structural imperfections that act as chemically active sites. Subsequent ultrasonic exfoliation and chemical functionalization with APTES introduce nitrogen-containing groups that preferentially interact with undercoordinated atoms and vacancy-adjacent regions generated during MXene delamination. These defect-rich regions provide energetically favorable anchoring environments for dopant incorporation, enabling the stabilization of nitrogen functionalities within the evolving MQD structure. During the hydrothermal cutting process that converts aminated nanosheets into quantum dots, the high density of edges and lattice discontinuities further amplifies defect availability, promoting the formation of coupled defect–dopant motifs. As a result, nitrogen dopants become integrated within defect-proximal sites rather than randomly distributed on pristine lattice domains, illustrating how structural imperfections formed during MQD generation can be actively utilized to engineer chemically stable and electronically tunable active sites.
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| Fig. 2 Schematic synthesis of N-doped MQDs from Ti3AlC2 highlighting defect formation and dopant incorporation during quantum cutting. This figure has been reproduced from ref. 44 with permission from Elsevier, copyright 2025. | ||
Unlike higher dopant concentrations, which may introduce disorder or nonradiative recombination pathways, single-atom dopants preserve structural integrity while enabling targeted functionality. This balance is particularly attractive for applications requiring high selectivity and reproducibility. From a synthetic standpoint, achieving single-atom doping in MQDs demands stringent control over precursor chemistry and reaction kinetics. Advances in bottom-up synthesis, precursor-limited growth, and in situ coordination control are making such precision increasingly feasible.28,44 The resulting MQDs challenge conventional compositional descriptors, as their properties cannot be averaged over dopant distributions. Instead, they necessitate atom-by-atom design logic, positioning single-atom-doped MQDs at the frontier of quantum materials engineering.
Fig. 3 provides structural and electronic evidence illustrating how ultrasmall MQDs create a suitable platform for precision engineering in the single-atom or ultra-low-concentration doping regime. Panel (a) outlines the synthesis pathway, where selective etching of the Al layer from Ti2AlC generates Ti2CTx MQDs decorated with surface functional groups. This process not only delaminates the layered precursor but also produces nanoscale domains enriched with chemically active surface sites. The TEM image in panel (b) shows highly dispersed MQDs with an average diameter of approximately 3 nm. At this dimension, the entire particle essentially operates within the quantum confinement regime, where the electronic structure becomes highly sensitive to atomic-scale perturbations. Consequently, the introduction of even a single heteroatom or a very small number of dopants can significantly influence the electronic behavior of the whole quantum dot, highlighting why such ultrasmall MQDs are promising hosts for atomically precise doping strategies.
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| Fig. 3 Structural and electronic characterization of Ti2CTx MQDs. (a) Schematic of HCl-etching synthesis route. (b) TEM image and size distribution (∼3 nm). (c) HRTEM showing lattice spacing of MQDs. (d) XPS spectra confirming removal of Al and formation of Ti–C bonds. (e) FTIR revealing surface functional groups. (f and g) Density of states of Ti2AlC and Ti2C MQDs showing Ti-3d dominated states near the Fermi level. This figure has been reproduced from ref. 69 with permission from Wiley Online Library, copyright 2023. | ||
Panels (c)–(g) further clarify the structural integrity and electronic characteristics that enable such precision engineering. The HRTEM image in panel (c) reveals well-defined lattice fringes corresponding to the (104) plane, indicating that the crystalline framework remains intact despite the extreme size reduction. Maintaining this structural order is essential because single-atom dopants interact strongly with the host lattice and their influence depends on well-defined local coordination environments. XPS spectra in panel (d) confirm the removal of Ti–Al bonds and the formation of Ti–C bonds, while FTIR analysis in panel (e) verifies the presence of surface functional groups such as –O and –OH. These groups can serve as coordination anchors that stabilize isolated heteroatoms or dilute dopant species. Finally, the density of states calculations in panels (f) and (g) show that Ti 3d orbitals dominate near the Fermi level, implying a high sensitivity of the electronic structure to local atomic modifications. Such sensitivity suggests that even a single dopant atom could introduce localized electronic states capable of modulating charge transfer dynamics. Nevertheless, it is important to note that while Fig. 1 establishes the structural and electronic framework conducive to single-atom doping, it does not directly visualize isolated dopant atoms; techniques such as HAADF-STEM or EXAFS would be required for definitive confirmation.
Edge-doped MQDs typically exhibit enhanced chemical accessibility due to the lower coordination numbers and higher surface energy of edge atoms. Dopants introduced at these sites can interact directly with the surrounding environment, facilitating rapid and selective binding events. In contrast, basal-plane doping tends to induce more subtle electronic modulation, influencing long-range charge transport and overall electronic stability.45,47 The choice between edge and basal-plane doping thus reflects a strategic trade-off between localized reactivity and global electronic control.
Recent advances emphasize spatially resolved doping strategies that combine both approaches within a single MQD. By independently tuning edge and basal-plane dopant populations, researchers can decouple reactivity from stability, enabling multifunctional MQDs.47,48 This level of spatial control underscores the evolution of MQD design from compositional tuning to architectural engineering at the atomic scale.
Importantly, the reduced dimensionality of MQDs amplifies these cooperative effects, making them particularly sensitive to dopant combinations. Moving beyond nitrogen-centric designs aligns MQD research with broader trends in quantum materials and single-atom catalysis. By embracing chemical diversity and atomic precision, heteroatom-doped MQDs can be engineered as customizable platforms rather than fixed compositions. This shift is essential for unlocking their full potential in advanced functional systems.51,52
Panel (A) in Fig. 4 schematically illustrates the controlled incorporation of chemically distinct dopants into Ti3C2 MQDs via an electrochemical etching strategy, highlighting the expansion of the dopant chemical space beyond nitrogen.52 In this system, nitrogen and chlorine are introduced through independent electrochemical pathways, selectively interacting with the carbon framework and titanium peripheries, respectively. Such spatially differentiated dopant incorporation demonstrates that MQDs can accommodate multiple heteroatoms with distinct electronegativity and bonding preferences within a single quantum-confined architecture. This co-doping strategy exemplifies how dopant diversity enables deliberate modulation of local electronic environments, moving MQD design beyond single-element doping toward chemically programmable systems.
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| Fig. 4 (A) Schematic illustration of the electrochemical fabrication of chlorine and nitrogen co-doped Ti3C2 MXene quantum dots with spatially differentiated dopant incorporation. (B) Conceptual representation of cooperative dopant-induced interfacial reactivity enabled by multi-element doping. This figure has been reproduced from ref. 52 with permission from Elsevier, copyright 2021. | ||
Panel (B) in Fig. 4 conceptually depicts the cooperative action of Cl and N dopants in regulating interfacial reactivity, serving as an example of emergent behavior arising from dopant–dopant coupling. Rather than acting independently, the coexistence of dopants with contrasting electronic character generates complementary charge redistribution pathways, enhancing the interaction of MQDs with reactive species. From a materials design perspective, this illustrates how co-doping can produce functionalities that are not accessible through nitrogen doping alone, underscoring the importance of expanding the dopant palette in MQDs.
Fig. 5 presents an integrated overview of the major atomic-level design strategies employed in heteroatom-doped MQDs. Unlike conventional compositional modification approaches, these strategies emphasize precise regulation of local electronic environments, defect distributions, and spatial dopant positioning within quantum-confined architectures. Dopant–host coupling and defect–dopant synergy collectively modulate charge redistribution and coordination behavior, while single-atom doping enables highly localized electronic control with minimal lattice disruption. In parallel, edge-selective and basal-plane doping introduce distinct reactivity and stability profiles, allowing decoupling of surface activity from global electronic transport. Multi-element co-doping further expands the accessible chemical space through cooperative electronic interactions between heteroatoms. Collectively, these atomic-level engineering approaches provide the structural and electronic foundation for enhanced selectivity, sensitivity, and multifunctionality in transition-metal ion sensing applications.
Table 1 provides a comparative overview of advanced atomic-level engineering strategies employed in heteroatom-doped MQDs. Rather than representing simple compositional modification, these strategies enable precise regulation of local electronic environments, defect distributions, and spatial dopant organization within quantum-confined architectures. Dopant–host coupling, defect-mediated electronic modulation, single-atom doping, and spatially selective edge/basal-plane engineering collectively govern charge redistribution, coordination behavior, and interfacial reactivity. In parallel, co-doping and chemical diversification strategies expand the accessible electronic and redox landscape of MQDs, enabling tailored recognition behavior toward transition-metal ions. Collectively, these approaches illustrate the evolution of MQD engineering from conventional bulk doping toward atomically programmable sensing architectures with tunable selectivity, stability, and multifunctionality.
| Design strategy | Dopant configuration | Spatial domain | Primary electronic effect | Structural/defect role | Functional outcome | Ref. |
|---|---|---|---|---|---|---|
| Dopant–host electronic coupling | N, S, P, B substitutional/interstitial doping | Edge + basal plane | Charge redistribution and orbital hybridization | Preserves lattice framework with localized perturbation | Tunable redox activity and selective ion coordination | 30–33 |
| Defect–dopant synergy | Vacancy-associated N/S doping | Vacancies and edge defects | Localized dipole formation and asymmetric charge density | Stabilization of defect-rich active sites | Enhanced affinity toward transition-metal ions | 34–36 |
| Single-atom doping | Isolated heteroatom incorporation | Edge or basal region | Discrete localized electronic states | Maintains structural integrity with minimal recombination | Ultra-selective and precision-controlled sensing | 37–39 |
| Low-concentration doping | Dilute N/S/P incorporation | Predominantly basal plane | Fine electronic band modulation | Reduced aggregation and defect-assisted stabilization | Improved photoluminescence stability/reactivity balance | 40–43 |
| Edge-selective doping | Edge-confined heteroatoms | MQD edge sites | High local charge density and surface reactivity | Exploits undercoordinated atomic environments | Rapid and accessible ion recognition | 43–46 |
| Basal-plane doping | Uniform basal-plane doping | Basal lattice region | Long-range electronic transport modulation | Minimal lattice distortion | Enhanced electronic stability and emission control | 47–50 |
| Multi-element Co-doping | N + S, N + P, B + S systems | Edge + basal combined | Synergistic charge polarization | Dopant–dopant electronic coupling | Multifunctional and enhanced sensing behavior | 50–52 |
| Heteroatom chemical expansion | Halogen, B, P, S incorporation | Edge/basal/interstitial | Electronegativity-driven orbital modulation | Cooperative structural stabilization | Expanded redox and analyte recognition capability | 42–44 |
| Spatially resolved doping | Segregated edge/basal doping | Architecturally differentiated MQDs | Decoupled reactivity and electronic transport | Selective defect utilization | Simultaneous stability and high chemical activity | 49–51 |
At the atomic level, the lattice structure consists of transition-metal layers sandwiched with carbon atoms, forming strong Ti–C bonds that provide structural stability and electronic conductivity. Surface terminations and edge defects introduce additional coordination sites capable of interacting with external species.20–22 These chemically active sites play a central role in ion recognition because they can coordinate with metal ions through electrostatic attraction, surface complexation, or electron-transfer processes.
Transition-metal ions such as Fe3+, Cu2+, Zn2+, and Co2+ possess partially filled d orbitals and well-defined coordination geometries. Their electronic configurations enable strong interactions with electron-rich surface groups on MQDs, particularly oxygen- or nitrogen-containing functional groups introduced through heteroatom doping. At the nanoscale interface, these ions may form coordination complexes with dopant atoms or surface ligands, leading to measurable changes in fluorescence, charge transfer, or electrochemical response.13–18
Therefore, understanding the atomic structures of both MQDs and transition-metal ions provides essential insight into the mechanisms of selective ion recognition. The interplay between the quantum-confined MXene lattice, surface functional groups, and the coordination chemistry of transition-metal ions ultimately governs sensing sensitivity and selectivity in heteroatom-doped MQD systems.
Ratiometric systems encode recognition events as signal ratios rather than absolute intensities, significantly improving accuracy in complex matrices. In the context of MQDs, this paradigm can be implemented through dual-emission systems, energy transfer cascades, or coupling MQDs with secondary emissive species. Importantly, the ratiometric concept is not merely a signal-processing upgrade but a fundamental shift in how recognition information is represented and interpreted. By converting chemical interactions into multidimensional optical outputs, these systems increase information density per sensing event.56,57
Beyond analytical reliability, ratiometric architectures enable discrimination between closely related analytes by exploiting differential modulation of multiple channels. This capability is particularly relevant for transition-metal ions, which often exhibit overlapping coordination behavior. By designing recognition systems that respond along orthogonal optical axes, MQD-based platforms can transcend the selectivity limitations of single-signal probes. At a systems level, ratiometric recognition aligns MQD sensing with broader trends in analytical chemistry toward self-referenced and error-tolerant measurement strategies.59–61 As sensing environments become increasingly complex—ranging from environmental samples to biological fluids—the transition from intensity-based to information-rich readouts represents a critical evolutionary step for MQD-enabled recognition technologies.
The panels in Fig. 6 illustrate the analytical performance of the MQD-based photoelectrochemical (PEC) aptasensor and highlight how signal modulation can encode recognition events with high reliability. Panel (A) shows the photocurrent responses obtained at different concentrations of lincomycin (Lin), where the gradual increase in signal reflects the sensitive interaction between the target molecule and the MQD-based sensing interface. This concentration-dependent modulation demonstrates how chemical recognition can be translated into measurable electronic outputs. Panel (B) presents the corresponding calibration relationship between photocurrent and the logarithm of Lin concentration, revealing a wide linear detection range and an ultralow detection limit, which indicates the high sensitivity of the sensing platform. Meanwhile, panel (C) evaluates the selectivity of the system by comparing the response to Lin with several structurally related antibiotics, confirming that the sensor maintains a highly specific response even in the presence of potential interferents. Finally, panel (D) demonstrates the operational stability of the aptasensor under repeated light on/off cycles, showing negligible signal degradation. Collectively, these results illustrate how MQD-integrated sensing architectures convert molecular recognition into reproducible and information-rich signal outputs, a key requirement for the development of robust and advanced recognition systems.
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| Fig. 6 Analytical performance of the PEC aptasensor. (A) Photocurrent responses at different Lin concentrations. (B) Calibration curve of photocurrent versus logarithmic concentration of Lin. (C) Selectivity evaluation against interfering antibiotics. (D) Stability test under repeated illumination cycles. This figure has been reproduced from ref. 60 with permission from Elsevier, copyright 2022. | ||
Stimuli-responsive behavior also enables reversible and reusable sensing systems. By designing recognition architectures that can switch between “on,” “off,” or intermediate states, MQD-based probes can perform multiple sensing cycles without structural degradation. This dynamic capability is particularly attractive for real-time monitoring applications, where continuous or repeated measurements are required. At a conceptual level, adaptive recognition represents a departure from single-analyte detection toward system-level responsiveness. MQDs serve not only as signal transducers but as integral components of responsive networks that process environmental information.65,66 This shift elevates MQD sensing from a passive measurement tool to an active analytical system capable of decision-making based on changing conditions.
Importantly, multimodal recognition does not simply replicate the same information across different outputs. Instead, each modality can be tailored to respond to distinct aspects of the recognition event, such as concentration range, kinetics, or competing species. This functional differentiation enhances the analytical depth of MQD-based systems and reduces ambiguity in real-world applications. From a translational perspective, multimodal strategies bridge the gap between laboratory-scale performance and field deployment. By accommodating both high-end instrumentation and low-resource settings, MQD-based multimodal sensors align with global trends toward decentralized and user-friendly analytical technologies. This versatility positions MQDs as adaptable platforms rather than single-purpose probes.69–71
Fig. 7 illustrates how the CPB–MXN quantum-dot composite operates as a platform capable of integrating optical excitation with electrical signal readout, highlighting the principles of multimodal recognition architectures. Panel (a) presents the device configuration used to probe the photoelectrical behavior of the QD films. The current–voltage curves in panel (b) show that individual CPB and MXN QD films exhibit weak electrical conductivity and limited photocurrent under illumination, indicating inefficient carrier transport and rapid recombination within isolated nanocrystals. In contrast, the CPB–MXN composite device in panel (c) displays markedly enhanced conductivity and a pronounced photocurrent response when illuminated. This behavior suggests efficient interfacial charge separation and transfer between CPB and MXN domains, which creates a conductive pathway that converts optical excitation into measurable electrical output. The dynamic photocurrent switching observed in panel (d) during repeated illumination cycles further confirms the reversible and stable photoresponse of the composite system. Together, these observations demonstrate how MQD-based hybrid structures can couple optical stimulation with electrical transduction, providing complementary signal channels that enhance detection reliability and analytical versatility. Such integration of photonic and electronic responses exemplifies the operational principle of multimodal sensing platforms, where different output modalities reinforce the interpretation of the same recognition event.
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| Fig. 7 (a) Device architecture of the CPB–MXN QD photodetector; (b) I–V characteristics of CPB and MXN QD films in dark and under illumination; (c) enhanced photocurrent response of the CPB–MXN composite device; (d) time-dependent photocurrent switching during repeated light on/off cycles. This figure has been reproduced from ref. 71 with permission from American Chemical Society, copyright 2020. | ||
Logic-gated recognition is especially valuable in environments containing multiple potential interferents. By encoding selectivity into logical conditions rather than relying solely on chemical affinity, MQD-based systems achieve higher specificity under realistic conditions. This strategy mirrors computational principles, effectively embedding basic information processing within the sensing material itself. At a broader level, logic-based recognition reflects the convergence of sensing and computation. MQD platforms capable of executing logical operations blur the boundary between analytical chemistry and molecular information science, opening pathways toward intelligent sensing systems that respond selectively based on predefined decision rules.42,72
Fig. 8 illustrates a sequential recognition process in which MQDs operate as a fluorescence transduction platform responding to two chemical inputs in a logic-like manner. As shown in panel (a), the FL intensity of MQDs is rapidly quenched upon the introduction of Ni2+, indicating the formation of a coordination interaction that suppresses emission. When histidine (His) is subsequently introduced, the fluorescence signal recovers due to the stronger complexation between Ni2+ and His, which disrupts the Ni2+–MQD interaction. This stepwise signal modulation demonstrates a sequential sensing mechanism in which the final output depends on the ordered introduction of two chemical species. Panel (b) further shows that the fluorescence recovery increases progressively with raising His concentration, reflecting the quantitative responsiveness of the system. The corresponding calibration curve in panel (c) confirms a linear relationship between fluorescence recovery and His concentration within the tested range, highlighting the analytical capability of the recognition architecture. Finally, panel (d) evaluates the selectivity of the system against other essential amino acids, demonstrating that significant fluorescence recovery occurs only in the presence of His. Together, these results exemplify how MQD-based sensing platforms can encode chemical events as ordered signal transformations, consistent with the principles of sequential and logic-gated recognition systems.
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| Fig. 8 Sequential fluorescence recognition of histidine using MQDs. (a) Time-dependent fluorescence response after sequential addition of Ni2+ and His. (b) Fluorescence recovery of Ni2+–MQDs at different His concentrations. (c) Calibration curve of fluorescence recovery versus His concentration. (d) Selectivity of the sensing system toward His over other amino acids. This figure has been reproduced from ref. 72 with permission from American Chemical Society, copyright 2021. | ||
Such integration is particularly relevant for continuous monitoring applications, where large volumes of data must be processed in real time. By coupling MQD-based sensors with computational tools, sensing platforms can adapt detection strategies dynamically, identify trends, and issue actionable outputs rather than raw signals. Ultimately, the evolution toward intelligent recognition systems redefines the role of MQDs in sensing technologies. They become components of adaptive analytical ecosystems rather than standalone probes. This paradigm shift aligns MQD research with broader movements toward smart materials and autonomous sensing infrastructures.75,76
Table 2 summarizes the evolution of MQD-based recognition systems from conventional single-channel fluorescence probes toward adaptive, multimodal, and data-integrated sensing architectures. Traditional intensity-based sensing provides operational simplicity but remains highly susceptible to environmental fluctuations and matrix-dependent interference. Emerging paradigms, including ratiometric, stimuli-responsive, multimodal, logic-gated, and sequential recognition systems, overcome these limitations by introducing self-calibration, dynamic signal modulation, and multidimensional analytical outputs. In parallel, intelligent data-integrated platforms combine MQD-generated signals with computational processing, enabling predictive analysis and autonomous sensing behavior. Collectively, these developments demonstrate the transformation of MQDs from passive fluorescence transducers into programmable and information-rich sensing systems capable of selective, adaptive, and real-time chemical recognition under complex operating conditions.
| Recognition strategy | Signal output | Recognition mechanism | Dynamic capability | Major analytical advantage | Application relevance | Ref. |
|---|---|---|---|---|---|---|
| Intensity-based fluorescence | Single-emission fluorescence | Direct quenching or enhancement | Static response | Simple and rapid signal generation | Conventional laboratory ion sensing | 53–55 |
| Ratiometric recognition | Dual-emission fluorescence | Ratio-based self-calibrated signaling | Internal referencing | Reduced environmental artifacts and enhanced quantification | Complex matrices and ion discrimination | 56–58 |
| Stimuli-responsive systems | Modulated fluorescence response | pH/ionic-strength/sequential control | Reversible adaptive sensing | Tunable sensitivity and reusable operation | Dynamic environmental monitoring | 59–61 |
| Multimodal recognition | Optical/electrochemical/visual outputs | Integrated multi-signal transduction | Parallel signal generation | Increased analytical confidence and reduced false positives | Portable and field-deployable sensing | 62–64 |
| Logic-gated recognition | Fluorescence/ratiometric outputs | Boolean or multi-input processing | Sequential input dependency | High specificity under interferent-rich conditions | Intelligent chemical recognition | 65–67 |
| Sequential recognition | Multi-step fluorescence modulation | Ordered analyte interaction pathways | Time-dependent response evolution | Improved discrimination fidelity | Multi-ion and complex sample analysis | 68–70 |
| Intelligent data-integrated platforms | Multivariate sensing signals | Algorithm-assisted signal interpretation | Real-time adaptive analytics | Predictive recognition and pattern analysis | Autonomous monitoring systems | 71–73 |
| FRET-based recognition systems | Energy-transfer fluorescence | MQD donor–acceptor interaction | Stimuli-dependent energy transfer | Multiplexed and orthogonal sensing capability | Bioimaging and multiplex detection | 74–76 |
In amino-functionalized Ti3C2Tx MQDs, Fe3+ recognition is dominated by redox interactions between the highly oxidizing Fe3+ ions and the electron-rich MQD surface. These interactions lead to efficient fluorescence quenching, producing a highly sensitive analytical signal with linear behavior spanning nanomolar to micromolar concentrations.77 Detection limits in the low nanomolar regime position such platforms well below regulatory thresholds for drinking water, making them particularly suitable for early-warning monitoring of iron contamination. The wide dynamic range further supports their applicability across diverse environmental conditions, from pristine water sources to industrial effluents.
Alternative MQD-based Fe3+ sensing strategies rely on electrostatic and aggregation-induced quenching effects rather than direct redox coupling. MQDs prepared through solvent-regulated ultrasonic routes exhibit rapid fluorescence suppression upon Fe3+ exposure, attributed to ion-induced aggregation processes that disrupt emissive pathways.78 Although these systems typically operate with micromolar detection limits, their rapid response kinetics and straightforward preparation protocols offer distinct practical advantages. Such characteristics are especially valuable for screening-level analyses or on-site testing scenarios where operational simplicity and speed are prioritized over extreme sensitivity. Taken together, these complementary approaches illustrate the adaptability of heteroatom-doped MQDs for Fe3+ monitoring. Redox-active platforms emphasize sensitivity and trace-level detection, while aggregation-driven systems favor robustness and ease of deployment.15,17 This performance diversity highlights how MQD-based Fe3+ sensors can be strategically selected or engineered to meet specific analytical objectives across varied environmental monitoring contexts.
As illustrated in Fig. 9A and C, the fluorescence emission of N-MQDs shows quenching behavior in the presence of Cu2+ ions; the same sensing platform was also reported to respond to Fe3+, indicating its multi-ion detection capability. With increasing metal ion concentration from 0.5 to 500 µM, the emission intensity decreases monotonically, indicating efficient interaction between the paramagnetic metal ions and the emissive states of the MQDs. In the case of Cu2+, this strong quenching response is attributed to the formation of stable coordination complexes between Cu2+ ions and amino functionalities introduced through nitrogen doping.60,61 Such coordination facilitates non-radiative electron or energy transfer processes, effectively depleting the excited-state population and suppressing fluorescence emission, consistent with a charge-transfer-assisted quenching mechanism.
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| Fig. 9 Fluorescence sensing performance of N-doped MQDs toward Fe3+ and Cu2+ ions. (A and C) Fluorescence emission spectra of N-MQDs recorded at 330 nm in the presence of increasing concentrations (0–500 µM) Cu2+ ion, respectively. (B and D) Linear relationship between normalized fluorescence quenching efficiency ((F0 − F)/F0) and metal ion concentration, demonstrating sensitive and quantitative detection in the low-concentration range. This figure has been reproduced from ref. 79 with permission from American Chemical Society, copyright 2022. | ||
Quantitative analysis of the sensing performance, shown in Fig. 9B and D, reveals a robust linear relationship between the normalized fluorescence quenching efficiency ((F0 − F)/F0) and Cu2+ concentration over the 0.5–100 µM range. The low detection limit of 0.15 µM underscores the high sensitivity achieved through heteroatom doping, which enhances both the intrinsic fluorescence intensity of the MQDs and their affinity toward Cu2+ ions. Compared with undoped MQDs, the aminated N-MQDs display significantly amplified quenching responses, highlighting the critical role of surface electronic structure and functional group engineering in regulating metal ion–MQD interactions. These results align well with the broader framework of fluorescence modulation and signal amplification, demonstrating how tailored MQD platforms enable reliable, selective, and ultrasensitive Cu2+ detection in aqueous environments.
In contrast, ratiometric MQD-based Cu2+ sensors encode ion recognition as a ratio between two fluorescence emissions, significantly enhancing analytical robustness.80 By decoupling the analytical signal from absolute intensity values, ratiometric amplification minimizes the influence of external variables such as excitation fluctuations, probe concentration variations, and photobleaching. As a result, detection limits are pushed into the nanomolar range, representing a substantial improvement in sensitivity and reliability compared to single-channel fluorescence probes.
From a performance perspective, intensity-based quenching sensors offer simplicity, broad dynamic ranges, and ease of implementation, making them suitable for routine monitoring applications. Ratiometric systems, while more complex, provide superior sensitivity and measurement stability, particularly in challenging or variable sample environments. Together, these complementary strategies establish heteroatom-doped MQDs as versatile and competitive platforms for Cu2+ detection across laboratory and real-world analytical scenarios.
In this system, Zn2+ coordination induces a pronounced fluorescence “turn-on” response, with linear detection behavior in the low micromolar range. The enhancement mechanism stems from stabilization of the excited-state electronic structure of the MQDs, promoting radiative recombination and suppressing non-radiative decay. This approach contrasts with conventional quenching-based sensors and allows Zn2+ to be detected with minimal interference from quenching-prone transition metals. The resulting analytical signal is highly sensitive, with low detection limits and good reproducibility across repeated measurements, demonstrating the robustness of the fluorescence enhancement strategy.81
A notable advancement of this platform is its sequential “off–on–off” modulation capability. After initial Zn2+-induced fluorescence enhancement, secondary analytes can modulate the emission reversibly, enabling multi-step sensing applications. This feature allows selective secondary detection without compromising Zn2+ quantification, which is particularly advantageous in complex sample matrices such as environmental waters and food extracts. By exploiting the reversible nature of coordination interactions, the platform integrates both primary detection and functional adaptability.17,61
The system's practical utility has been validated in real-world matrices, highlighting the potential of fluorescence enhancement-based MQDs for operationally relevant Zn2+ sensing. Compared to redox- or quenching-dominated platforms, this strategy provides superior selectivity in mixed-metal environments, where non-redox ions would otherwise fail to produce measurable or distinguishable signals. Overall, the approach illustrates how diversifying signal transduction modes broadens the functional capabilities of MQD-based sensors, establishing a pathway for analytically challenging ions to be detected with high fidelity.
The ratiometric approach also confers superior selectivity in complex ionic matrices, where competing divalent cations or varying ionic strength might otherwise compromise detection. Testing in commercially available mineral waters confirmed both high selectivity and reproducibility. Importantly, the platform can be translated into visual and portable formats, such as test strips, enabling rapid on-site analysis without the need for sophisticated instrumentation. This combination of sensitivity, selectivity, and deployability addresses the growing demand for practical water quality monitoring tools. From a design perspective, ratiometric MQDs exemplify how heteroatom doping and engineered emission properties can overcome intrinsic sensing limitations of chemically inert or weakly interacting metal ions. By leveraging dual-emission behavior and internal referencing, these systems maintain analytical fidelity while broadening applicability beyond laboratory conditions.53,60 The Mn2+ platform thus establishes a generalizable framework for incorporating ratiometric signal strategies into next-generation MQD-based metal ion sensors.
Fig. 10 systematically illustrates the design rationale and analytical robustness of the dual-emission ratiometric MQD-based probe (MQDs–EDTA–Eu3+–DPA) for Mn2+ detection. Optimization of experimental parameters reveals that both Eu3+ concentration and solution pH critically govern sensing performance. As shown in Fig. 10A, the ratiometric response toward Mn2+ is maximized at a Eu3+ concentration of 100 µM, where balanced emission intensities enable optimal signal contrast. Meanwhile, Fig. 10B and C demonstrate that near-neutral pH conditions favor stable and reproducible detection of Mn2+ ion, justifying the use of PBS buffer at pH 7.0 for subsequent measurements. This optimization step is essential for ensuring that ratiometric outputs reflect genuine metal–probe interactions rather than environmental fluctuations.
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| Fig. 10 Ratiometric fluorescence sensing of Ca2+ and Mn2+ using the MQDs–EDTA–Eu3+–DPA probe. (A) Effect of Eu3+ concentration on detection sensitivity. (B and C) Influence of pH on Ca2+ and Mn2+ sensing performance. (D) Dual-emission fluorescence spectra and (E) corresponding ratiometric calibration curve (IF616/IF445) for Ca2+ detection. (F) Selectivity evaluation in drinking water matrices. (G) Fluorescence spectra and (H) ratiometric calibration curve (IF380/IF616) for Mn2+ detection. (I) Selectivity evaluation in natural mineral water matrices. Insets: fluorescence photographs before and after addition of Mn2+. This figure has been reproduced from ref. 82 with permission from Fxcsxb, copyright 2025. | ||
Under UV excitation at 265 nm, the probe exhibits two well-resolved emission bands: a blue emission at 445 nm originating from the MQDs and a red emission at 616 nm associated with the Eu3+–DPA complex (Fig. 10D). Upon addition of Ca2+ ions, the red Eu3+-centered emission is selectively attenuated while the MQD emission remains invariant, yielding a visually discernible color transition from red to light blue (inset of Fig. 10D). The resulting linear relationship between IF616/IF445 and Ca2+ concentration (Fig. 10E) confirms the role of the MQD emission as an internal reference channel, highlighting the self-calibrating nature of the ratiometric strategy.
In contrast, Mn2+ detection proceeds through a distinct dual-modulation pathway. As shown in Fig. 10G, coordination between Mn2+ ions and DPA ligands induces the emergence of a new purple emission band at 380 nm, attributed to the Mn2+–DPA complex, while the Eu3+-based emission at 616 nm is gradually suppressed. This dual-emission evolution produces a clear color change from red to purple (inset of Fig. 9G) and enables construction of a highly linear ratiometric calibration curve based on IF380/IF616. The low detection limit in the nanomolar regime underscores the effectiveness of ratiometric amplification in overcoming the inherently weak fluorescence perturbation typically associated with Mn2+ ions.
Selectivity studies further validate the analytical reliability of this platform. As depicted in Fig. 10F and I, common coexisting ions defined in drinking water and natural mineral water standards induce negligible interference in the ratiometric response. This resistance to matrix effects, combined with internal referencing and visually distinguishable fluorescence changes, exemplifies how dual-emission MQD architectures can deliver high-fidelity Mn2+ sensing under realistic conditions.
The platform exemplifies a performance balance that extends MQD applicability beyond ultra-trace detection. By engineering MXene composition and heteroatom dopants, the sensing system achieves a combination of moderate sensitivity, functional stability, and application versatility. This approach underscores the importance of tailoring MQD materials to meet multi-dimensional requirements, such as compatibility with biological environments, optical robustness, and simultaneous analytical and imaging capabilities.40,53 Overall, Nb2C MQDs highlight a strategic route for expanding MQD-based sensors to alternative transition-metal targets, demonstrating that material diversity can unlock multifunctional sensing performance. These findings reinforce the broader potential of heteroatom-doped MQDs to serve as flexible, tunable platforms for selective transition-metal ion recognition, bridging environmental and bioanalytical applications.
As shown in Table 3, the differences in analytical performance among heteroatom-doped MQD-based sensors, particularly in terms of detection limit, are closely related to their structural design, surface chemistry, and signal-output mode. Sensors exhibiting nanomolar-level LODs generally benefit from stronger and more specific interactions between the target metal ions and the doped MQD surface. In this context, heteroatom doping creates defect-rich active sites and modulates the electronic structure of MQDs, which enhances charge transfer and fluorescence responsiveness upon metal-ion binding. At the same time, surface functional groups such as amino, hydroxyl, or sulfur-containing moieties improve coordination affinity and contribute to higher selectivity. Table 3 also indicates that sensing platforms based on FRET or ratiometric fluorescence often achieve superior sensitivity compared with conventional single-intensity quenching systems, because they reduce background interference and improve signal precision. Therefore, lower detection limits are not determined by a single factor, but rather by the synergistic combination of dopant engineering, interfacial recognition chemistry, and advanced signal transduction strategies.
| MQDs type/modification | Target analyte | Detection strategy | Linear range | LOD | Key notes | Ref. |
|---|---|---|---|---|---|---|
| Amino-functionalized Ti3C2Tx MQDs | Fe3+ | Fluorescence sensing | nM to µM range | 2 nM | Ultrasensitive detection via redox interaction between Fe3+ and Ti3C2Tx MQDs | 77 |
| MXene QDs regulated by DMF | Fe3+ | Aggregation-induced fluorescence quenching | Not specified | 1.4 µM | Sensitivity: 0.6377 mM−1 | 78 |
| Covalently N-doped Ti3C2 MQDs | Fe3+/Cu2+ | Fluorescence sensing | 0.5–500 µM | 0.17 µM (Fe3+); 0.15 µM (Cu2+) | Amino-rich surface improves sensitivity and stability | 79 |
| N-doped Ti3C2 MQDs | Cu2+/D-penicillamine | FRET-based ratiometric fluorescence | Not specified | 3.0 nM (Cu2+); 0.115 µM (D-PA) | Ratiometric fluorescence based on ox-OPD formation | 80 |
| N-doped MQDs | Zn2+/oxalic acid | “Off–On–Off” fluorescence sensing | 0–20 µM | 0.127 µM (Zn2+); 0.883 µM (OA) | ICT mechanism with Zn2+ and coordination with OA | 81 |
| MQDs–EDTA–Eu3+–DPA probe | Ca2+/Mn2+ | Ratiometric fluorescence | Not specified | Not specified | Dual-emission probe using antenna effect | 82 |
| S,N-co-doped Nb2C MQDs | Cu2+ | Fluorescence sensing | Not specified | 2 µM | Also applied in cell imaging | 83 |
In addition, the ion selectivity observed in different MQD-based sensing systems originates from several structural and chemical factors associated with the quantum dots. The specificity toward particular metal ions is largely governed by the composition of the MQDs, the type of heteroatom dopants, and the surface functional groups introduced during synthesis. Heteroatom doping can tailor the electronic structure and create defect-rich active sites that preferentially interact with certain metal ions through charge transfer or coordination processes. At the same time, surface functional groups such as amino, hydroxyl, sulfur-containing, or carboxyl moieties provide coordination environments with different binding affinities for specific ions. The synthetic methodology also plays an important role because it controls particle size, defect density, dopant distribution, and surface termination of MQDs. Consequently, variations in synthesis conditions and surface chemistry lead to distinct host–guest interactions with target ions, enabling MQD sensors to achieve selective detection of different metal ions across various sensing platforms.
One widely adopted approach involves masking strategies, where specific reagents selectively complex interfering ions and reduce their effective participation in the sensing process. By suppressing competing interactions, masking agents reshape the ionic environment encountered by MQDs and improve discrimination toward the target analyte.78–80 This strategy reflects the practical reality that many transition metals exhibit overlapping coordination chemistry, making perfectly exclusive binding difficult to achieve at the material level.
Another emerging route involves differential signal modulation. In these systems, different metal ions produce distinct optical responses, such as fluorescence quenching, enhancement, wavelength shifts, or the generation of secondary emission bands. Rather than relying on a single binary response, MQD probes can therefore generate response patterns that allow discrimination between ions based on their optical fingerprints.
Although simultaneous multi-ion detection using MQD platforms is still relatively limited, these strategies provide practical routes for operating MQD sensors in complex ionic matrices. Approaches such as masking, ratiometric normalization, sequential sensing protocols, and controlled reagent addition can collectively improve analytical selectivity. Consequently, selectivity engineering is increasingly viewed not only as a property of the MQD material itself but also as a function of the overall sensing workflow and measurement design.
Visual and semi-quantitative detection strategies represent an important step toward field-applicable sensing. In several MQD-based systems, fluorescence responses can be translated into colorimetric or visually discernible outputs, enabling rapid screening without sophisticated instrumentation.79–82 Test-strip formats, paper-based analytical devices, and simple fluorescence readouts have been explored as preliminary approaches for on-site detection, demonstrating the potential of MQDs for portable sensing platforms.
At the same time, achieving reliable performance under real environmental conditions requires robustness against fluctuations in pH, ionic strength, temperature, and sample composition. Such robustness is often achieved through system-level design, including protective matrices, internal referencing strategies, and controlled sensing environments. These developments highlight that practical sensing performance depends not only on the MQD material itself but also on the overall integration of the sensing platform.
Although fully deployable MQD-based sensing devices are still limited, current studies illustrate early steps toward portable and application-oriented systems. Continued integration of MQDs with simple analytical formats, portable detection tools, and application-specific workflows is expected to facilitate their transition from laboratory demonstrations to practical sensing technologies for environmental monitoring, food safety assessment, and bioanalytical screening.
Another challenge involves selectivity in complex matrices. While many MQD sensors demonstrate excellent selectivity under controlled laboratory conditions, real environmental and biological samples often contain multiple competing ions, organic molecules, and fluctuating physicochemical parameters. Under such circumstances, nonspecific interactions or matrix-induced fluorescence perturbations may reduce analytical accuracy.48–50 Consequently, strategies such as ratiometric detection, masking agents, and internal referencing are increasingly employed to mitigate interference effects.
Long-term stability also represents an important consideration for practical applications. MQDs may undergo gradual surface oxidation, ligand detachment, or photobleaching during prolonged storage or repeated measurements. These processes can alter fluorescence intensity and sensing response over time, highlighting the need for improved surface passivation and protective matrices.
Finally, although MQD-based sensors have achieved impressive detection limits in laboratory studies, translation into scalable and field-deployable devices remains limited. Integration with portable sensing formats, standardized synthesis protocols, and robust validation in real-world samples will be essential for advancing MQD technologies toward routine environmental and bioanalytical monitoring. Addressing these challenges will help bridge the gap between promising laboratory demonstrations and reliable practical sensing systems.
Within this broader landscape, MXene-derived quantum dots present a distinct class of fluorescent nanomaterials characterized by abundant surface terminations, strong electron transfer capability, and versatile chemical tunability. These features facilitate efficient interactions with metal ions through surface functional groups and defect sites, often leading to pronounced fluorescence quenching or enhancement responses. Compared with many conventional nanosensors, MQDs can provide rapid signal transduction and flexible surface modification through heteroatom incorporation, enabling selective recognition of specific metal ions.
Despite these advantages, MQD-based sensing systems are still developing compared with more established fluorescent nanomaterials. Several studies have reported excellent sensitivity and promising selectivity toward targeted ions, yet systematic comparisons across different nanomaterial platforms remain relatively limited.49–81 Therefore, placing MQD-based sensors within the broader family of fluorescent nanosensors helps clarify their emerging role, highlighting both their unique advantages and the areas where further optimization and comparative evaluation are still required.
In addition to these broader perspectives, several fundamental bottlenecks continue to limit the practical implementation of MQD-based ion sensing systems. One key challenge is batch-to-batch reproducibility during MQD synthesis, where slight variations in precursor composition, etching conditions, or heteroatom incorporation can significantly alter particle size, defect density, and surface functional groups. These structural variations often translate into inconsistent fluorescence responses and ion-binding behavior, complicating quantitative sensing. Another concern is long-term stability. MQDs may undergo gradual oxidation, surface ligand rearrangement, or photobleaching during storage and repeated measurements, potentially leading to signal drift over time. Furthermore, although many MQD probes demonstrate excellent selectivity under controlled laboratory conditions, their performance can deteriorate in complex matrices containing competing metal ions, organic ligands, and fluctuating physicochemical parameters. These limitations highlight the importance of standardized synthesis protocols, systematic stability evaluation, and robust selectivity engineering to ensure reliable analytical performance in practical sensing environments.
A major constraint in current MQD research is the scalability of synthesis. Most high-performance sensors rely on hydrothermal, ultrasonic, or chemical exfoliation protocols optimized for milligram-scale production. While these approaches produce monodisperse, heteroatom-functionalized MQDs with high quantum yields, their translation to gram- or kilogram-scale quantities remains underexplored. Batch-to-batch variability, precursor costs, and reaction reproducibility are significant hurdles. For instance, nitrogen-doped Ti3C2 MQDs achieve ultralow detection limits for Fe3+ through surface redox interactions, yet the reproducibility of amino-functionalization in large batches remains uncertain. Emerging strategies, such as continuous-flow hydrothermal reactors or automated ultrasound-assisted synthesis, offer potential routes for scale-up while maintaining particle uniformity and surface chemistry fidelity. However, systematic studies quantifying the trade-offs between throughput, quantum yield, and doping efficiency are still scarce.64,80 Addressing these synthesis bottlenecks is essential for enabling industrial-scale production and widespread deployment of MQD-based sensors.
Equally critical is the fundamental selectivity limit of MQD systems. While heteroatom doping—such as N-, S-, or co-doping—provides tunable coordination sites for target ions, real-world samples present highly complex ionic matrices. Competitive binding, ion pairing, and nonspecific interactions can significantly alter fluorescence responses, particularly for chemically inert ions like Zn2+ or Mn2+. Traditional strategies often rely on masking agents, ratiometric normalization, or sequential detection protocols to enhance selectivity. Yet, these approaches have inherent limitations: masking agents may themselves interfere under multi-component conditions, and ratiometric readouts may not fully compensate for subtle matrix effects. Furthermore, the chemical design of MQD surfaces often faces trade-offs between selectivity and quantum yield, where extensive functionalization can quench emission or destabilize colloidal suspensions.71,82 A critical future direction involves integrating computational design and machine-learning-assisted screening to predict optimal heteroatom arrangements and binding motifs. This would allow rational tuning of surface sites for maximal selectivity against specific ion panels, rather than relying solely on empirical optimization.
In addition to machine-learning-assisted materials screening, density functional theory (DFT) calculations can provide critical atomic-level insights into the sensing behavior of heteroatom-doped MQDs. Computational studies can elucidate how dopant identity, concentration, and spatial distribution influence electronic band structures, charge-density redistribution, adsorption energies, and metal-ion binding affinity. For example, DFT-derived density of states (DOS) analysis may reveal how N- or S-doping introduces localized electronic states near the Fermi level, thereby facilitating charge transfer interactions with transition-metal ions such as Fe3+ or Cu2+. Similarly, adsorption-energy calculations can help identify preferential ion-binding sites and predict selectivity trends under competitive conditions. Integrating DFT analysis with experimental fluorescence and electrochemical observations would significantly strengthen mechanistic interpretation and support the rational design of MQD sensing architectures with optimized selectivity, stability, and electronic performance.
Beyond the current strategies, several material-level approaches could further enhance the sensing performance of MQD-based platforms. A particularly promising direction involves precise engineering of heteroatom distribution and defect structures within the MQD lattice. Instead of relying on random doping, future research could focus on controlled co-doping or the creation of single-atom active centers that generate highly selective coordination environments for specific transition-metal ions. Such atomic-scale design can significantly strengthen charge-transfer interactions between MQDs and target ions, leading to amplified fluorescence modulation and improved analytical sensitivity. Additionally, systematic control of MQD size distribution, edge termination, and surface passivation may enhance quantum yield and photostability, both of which are critical parameters for achieving ultralow detection limits. Integrating computational modeling and machine-learning-guided material design could further accelerate the discovery of optimized MQD structures with tailored electronic properties and selective binding motifs.
At the sensing architecture level, future research should also prioritize the development of advanced signal-transduction strategies that overcome the limitations of conventional single-intensity fluorescence quenching. Ratiometric fluorescence systems, fluorescence lifetime-based sensing, and FRET-mediated energy transfer platforms can significantly improve analytical accuracy by minimizing background interference and environmental fluctuations. Moreover, constructing hybrid nanostructures—such as MQD–metal nanoparticle, MQD–polymer, or MQD–MOF composites—may enhance sensitivity through synergistic electronic and plasmonic interactions. These innovations could enable multiplexed ion detection and real-time monitoring in complex matrices. In this context, integrating MQD sensing elements with portable analytical devices and IoT-enabled platforms may facilitate automated data acquisition and continuous environmental monitoring, transforming MQD-based probes from laboratory demonstrations into intelligent sensing systems capable of large-scale, real-world deployment.
Operational robustness and matrix adaptability constitute another essential axis for real-world deployment. Laboratory-based demonstrations often use buffered aqueous solutions or minimal ionic backgrounds, which do not reflect the variability encountered in drinking water, industrial effluents, or biological fluids. MQD performance under varying pH, ionic strength, temperature, and organic content is highly sensitive, potentially leading to false positives or signal drift. Recent trends highlight dual-emission ratiometric probes, sequential “off–on–off” signal modulation, and test-strip formats as promising strategies for maintaining reliable readouts across variable conditions.56,78 However, systematic evaluation under standardized protocols is limited. Future research should establish performance benchmarks that incorporate environmental variability, mimicking real matrices to assess robustness and reproducibility comprehensively.
Future research on MQD-based ion sensing should move beyond general performance improvement and focus on several concrete development directions. One promising approach is the controlled engineering of MQD surface terminations and heteroatom doping to regulate charge transfer interactions with specific metal ions, enabling more predictable sensing responses. Another important direction involves designing MQD composites with polymer matrices, porous substrates, or microfluidic platforms to improve probe stability and facilitate integration into portable sensing devices. Additionally, systematic studies that correlate MQD structure, surface chemistry, and fluorescence behavior are needed to clarify sensing mechanisms and guide rational sensor design. The development of standardized synthesis protocols may also improve reproducibility and allow more reliable comparison between studies. Finally, expanding investigations toward complex environmental and biological matrices will be essential for validating the practical applicability of MQD-based fluorescent probes under realistic analytical conditions.
A critical frontier lies in deployable sensor architectures that bridge laboratory performance with field applicability. Portable platforms, including lateral-flow devices, microfluidic chips, and smartphone-assisted fluorescence readers, are gaining attention. Visual readouts derived from colorimetric conversion of MQD fluorescence or ratiometric dual-emission systems offer low-cost, user-friendly options suitable for decentralized monitoring. Integrating MQDs with solid supports, polymer matrices, or paper-based substrates can improve colloidal stability and facilitate practical handling. Nevertheless, maintaining sensitivity and selectivity during immobilization remains challenging, particularly when heterogeneous matrices alter diffusion kinetics or binding equilibria.80,83 Advances in surface engineering, encapsulation chemistry, and device integration are therefore critical to achieve scalable, reliable, and user-oriented detection platforms.
Biocompatibility and multifunctionality represent an additional dimension, especially for applications intersecting biomedical imaging and ion detection. Certain Nb2C- and Ti3C2-based MQDs demonstrate dual utility in live-cell imaging and metal ion sensing, highlighting their potential for simultaneous diagnostic and monitoring applications. However, the long-term cytotoxicity, metabolic clearance, and biodistribution of heteroatom-doped MQDs remain largely unexplored. Future studies must systematically quantify biocompatibility while optimizing emission efficiency, surface passivation, and functional stability. The convergence of sensing and imaging applications could redefine the scope of MQD technologies, enabling simultaneous environmental and biological monitoring in a single platform.
From a broader perspective, data-driven integration and multiplexing will likely dictate the next generation of MQD-based sensors. The ability to discriminate between multiple ions within complex matrices using multidimensional fluorescence readouts, combined with real-time analytics, offers a path toward smart sensing networks. Pattern recognition, fluorescence lifetime mapping, and FRET-based ratiometric encoding could enhance selectivity and provide simultaneous multi-ion detection.77,81 Furthermore, combining MQD sensing platforms with IoT-enabled devices could allow automated, continuous monitoring, providing actionable environmental or biomedical insights.
While heteroatom-doped MQDs demonstrate exceptional promise for selective transition-metal ion detection, translating laboratory performance into practical, scalable, and reliable technologies requires addressing several critical challenges: scalable synthesis, fundamental selectivity limits, environmental robustness, device integration, and multifunctional applicability. Advances in automated synthesis, rational surface design, ratiometric and sequential signaling, portable device engineering, and smart analytics collectively define the future trajectory of MQD-based sensors.79,82 By systematically integrating these strategies, the field can progress from high-performance proof-of-concept studies to next-generation analytical tools capable of real-world environmental monitoring, biomedical diagnostics, and industrial quality control, positioning MXene QDs as a cornerstone of emerging quantum-dot-based sensing technologies.
Critical challenges remain in scalability, matrix adaptability, and real-world deployment. Laboratory-optimized MQDs must overcome synthesis reproducibility limitations, maintain selectivity under competitive binding conditions, and integrate into portable, user-friendly devices for field applications. Future research should emphasize rational heteroatom placement, multidimensional signal interpretation, and system-level engineering, including test-strip, microfluidic, and IoT-integrated platforms. Overall, MQDs represent a next-generation sensing platform that unites sensitivity, selectivity, and multifunctionality. By addressing current limitations and leveraging material diversity, MQD-based sensors are poised to transition from proof-of-concept studies to robust, deployable analytical tools, with broad implications for environmental monitoring, water quality assessment, and biomedical diagnostics. Their tunable optical properties, modular design, and adaptability firmly establish heteroatom-doped MQDs as a leading technology in advanced ion sensing research.
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