Open Access Article
Fang Li
a,
Panpan Dongb,
Zijian Wu
*bcd,
Lu Xueb,
Mingming Luob and
Yijun Tanb
aSchool of Information Engineering, Tianjin University of Commerce, Tianjin, 300134, China
bTianjin Key Laboratory of Food Biotechnology, College of Biotechnology and Food Science, Tianjin University of Commerce, 409, Guangrong Road, Tianjin, 300134, China. E-mail: wzjian@tjcu.edu.cn; Tel: +86-18622219597
cKey Lab of Agricultural Products Low Carbon Cold Chain, Ministry of Agriculture and Rural Affairs, Tianjin, 300134, China
dTianjin Key Laboratory of Edible Probiotics, Tianjin, 300134, China
First published on 17th September 2025
As ubiquitous pollutants, heavy metal ions can accumulate in the food chain, increasing toxicity through synergistic effects and posing health risks to humans and other organisms. In this study, we successfully developed a dual-signal aptasensing interface for simultaneous detection of cadmium ions (Cd2+) and lead ions (Pb2+). The 2D layered Ti3C2 MXene and liquid exfoliated graphene (LEG) composite nanomaterials were employed as ITO electrode modification materials, which exhibited enhanced electrochemical properties. The Cd2+-specific aptamer labeled with Nile blue and Pb2+-specific aptamer labeled with ferrocene bind to their complementary strands immobilized on the electrode surface, resulting in a dual-signal interface. In the presence of target ions, the aptamers specifically recognized and captured the targets, subsequently detaching from the electrode surface, leading to changes in the dual-signals and thereby enabling simultaneous detection of Cd2+ and Pb2+. The limits of detection for Cd2+ and Pb2+ were determined to be 0.689 pM and 1.548 pM, with linear response ranges of 0.1 pM to 10 μM and 0.01 pM to 10 μM. The effectiveness of the proposed aptasensor in determining Cd2+ and Pb2+ simultaneously in water and vegetables has been demonstrated, providing substantial evidence for its potential application in food safety and environmental monitoring.
In the contemporary era, a plethora of well-established techniques have become prevalent in the field of metal ion analysis, including Cd2+, Pb2+, and others. These include atomic absorption spectrometry,5 atomic emission spectrometry,6 X-ray fluorescence spectroscopy,7 inductively coupled plasma mass spectrometry,8 surface enhancement Raman scattering,9 and colorimetric methods.10 Among these, the atomic absorption spectrometry technique has become a standard analytical method for the determination of heavy metal ions due to its good sensitivity, excellent selectivity, and high accuracy. However, it should be noted that such methods are not without their limitations, frequently requiring large-scale instrumentation, complicated operation procedures, and high levels of expertise, which can be costly and time-consuming and may not always meet the requirements of on-site monitoring. Conversely, the colorimetric method offers several advantages, including ease of operation and intuitive results, which are conducive to immediate on-site detection. However, the majority of contemporary colorimetric methods for the determination of Cd2+ and Pb2+ do necessitate biologically active substances, which directly results in an increase in the cost of detection and the difficulty of sample preservation.3
In recent years, electrochemical sensors have attracted significant attention in the field of heavy metal ion detection, due to their clear advantages over traditional methods. Electrochemical sensors achieve quantitative detection by converting detected signals into electrical signals, including current, potential, resistance, and other electrochemical signals.11,12 A substantial body of research has demonstrated the merits of this technique, including its simplicity, portability, cost-effectiveness, rapid analysis, low detection limit, sensitivity, and selectivity.13,14 Nanomaterials are frequently introduced to enhance the sensitivity and selectivity of electrochemical sensors, and obtain a lower limit of detection (LOD). It is important to note that the performance of the sensor in detecting Cd2+ and Pb2+ is influenced by the type of nanomaterial used. For instance, Nguyen employed gold nanoparticles bearing sodium thiosulfate and surfactant-caps to detect Pb2+ with a detection limit of 20 nM.15 After that, Guo utilized Au@Pd bimetallic nanoparticles for Pb2+ detection, achieving a detection limit as low as 0.4 nM.16 It is noteworthy that the discrepancy in detection limits between these two methods can reach up to 50 times. The range of available nanomaterials is broad, including metal and oxide metal nanoparticles (NPs),17 carbon-based nanomaterials,18 conductive polymers,19 and semiconductors.20 In recent years, transition metal carbides/carbon-nitrides (MXenes) as a particularly promising class of two-dimensional material, exhibit unique electrical and interfacial properties, such as high conductivity, large specific surface area, and excellent chemical stability.21–23 The flake surface is rich in functional group sites, which allow for the flexible modulation of surface properties through chemical modifications.4,24 Meanwhile, carbon-based materials, such as graphene oxide and carbon nanotubes (CNTs), are of significant importance in the field of electrochemical sensors due to their properties and diverse structures. For example, Zukauskas et al. developed an electrochemical sensor based on layered Ti3C2Tx MXene for the detection of Pb2+ in solution, the sensor demonstrated a linear response within the range of 0.15–1.0 μM, exhibiting a sensitivity of 26.7 μA μM−1 and a detection limit of 48.7 nM.25 The sensor's functionality in real-time environmental monitoring underscores the potential of MXene-based sensors for environmental monitoring and public health applications, characterised by their rapid, portable and cost-effective nature. Notably, graphene, with its two-dimensional structure, has garnered significant attention due to its exceptional electrical conductivity, substantial specific surface area, notable mechanical flexibility, self-assembling activity, and remarkable chemical and electrochemical stability.26–28 Liang et al. reported an electrochemical sensor based on reduced graphene oxide (rGO) for the efficient detection of Cd2+.29 The sensor demonstrated exceptional electron transfer capability, immune to interference, stability, repeatability and reproducibility over the range of 0.92 μg L−1 to 36.7 mg L−1 with a detection limit of 0.478 μg L−1. Furthermore, it exhibited high recoveries (99.4–102.3%) in real water and rice samples. However, only Ti3C2 MXene or graphene exhibits a propensity for stacking, which is a subject of concern. This work proposes an effective strategy to dope LEG into Ti3C2 MXene. The utilisation of ultra-thin LEG nanosheets facilitates the interfacial charge transfer in electrochemical reactions, while the introduction of LEG effectively prevents the agglomeration of Ti3C2 MXene, thereby ensuring the retention of its favorable electrical conductivity and mechanical properties.
In order to enhance the selectivity capability of these sensors, there has been a recent focus on the integration of organic small molecule probes, proteins, enzymes and DNA probes into the existing electrochemical detection systems.30 Among these, DNA has attracted much attention due to its chemical stability, ease of mass production and high commercial value. An aptamer is a functional single-stranded DNA or RNA oligonucleotide obtained by in vitro screening that is able to form a specific spatial structure by binding to the target through hydrogen bonding, hydrophobic interactions, electrostatic interactions and van der Waals forces. Following binding to the target, the aptamer folds into a unique three-dimensional structure, a process known as ‘wrapping’ the target molecule.31 This is accompanied by an increase in the efficiency of electron transfer between the redox marker and the electrode, resulting in the amplification of the assay signal and the sensitive detection of the target. For instance, in the detection of Pb2+, guanine (G)-rich oligonucleotides can be converted to G-quadruplex structures through the induction of Pb2+. This conformational change provides great flexibility in designing electrochemical aptasensors. When the aptamer is labelled and immobilised with a redox group (e.g. ferrocene, methylene blue or Nile blue), the conformational change that occurs upon binding the analyte shortens the distance between the redox label and the electrode. This, in turn, induces a change in the current response, which leads to the development of high-performance electrochemical aptasensors.
In this study, the innovative choice of LEG@Ti3C2 MXene to modify indium tin oxide (ITO) electrodes is examined.32 ITO has become one of the most widely used conductors due to its excellent conductivity and high transparency, and its surface can be precisely modified by many cutting-edge technologies.33–36 The highly specific affinity between the aptamer and the metal ions was exploited for the sensitive detection of Cd2+ and Pb2+ simultaneously. As illustrated in the scheme diagram, the amino group (–NH2) present on the complementary chain of the metal ion aptamer interacts with the carboxyl group (–COOH) on the surface of the LEG@Ti3C2 MXene, thereby facilitating the efficient assembly of the aptamer on the LEG@Ti3C2 MXene/ITO electrode. It is noteworthy that the Cd2+ and Pb2+ aptamers, which are labeled with Nile blue and ferrocene, respectively, can be firmly attached to the LEG@Ti3C2 MXene/ITO electrode by virtue of the base complementary pairing. Initially, in the absence of Cd2+ and Pb2+ ions, the sensor displays a high-intensity electrochemical signal. However, upon the introduction of Cd2+ and Pb2+, the metal ions bind specifically to the aptamers, causing a dissociation of the rigid double-chain structure and a subsequent movement of the aptamers away from the gold electrode. This results in a weakening of the electrochemical signal of the modified electrode. The dynamic changes in peak current before and after recognition can be used for quantitative evaluation of Cd2+ and Pb2+ simultaneously.
Ferrocene carboxylic acid, 1-thyl-3-[(3-dimethylamino)propyl] carbodiimide (EDC), N,N′-dicyclohexylacrbodiimide (DCC), N-hydroxysuccinimide (NHS), 3-(N-morpholino) propane sulfonic acid (MOPs), Nile blue (NB) and CaCl2 were procured from Shanghai Yuanye Bio-Technology Co., Ltd (Shanghai, China). CdCl2, Co(NO3)2, CuCl2, MnCl2, PbCl2, and FeCl2 were procured from Shanghai Macklin Biochemical Co., Ltd (Shanghai, China).
The synthesis of Ti3C2 MXene nanosheets was conducted in accordance with the method previously reported.38 Initially, 1 g of Ti3AlC2 and 1.8 g of lithium fluoride were homogeneously dispersed in 20 mL of hydrochloric acid at a concentration of 9 M. The mixture was then stirred for 26 h at a constant temperature of 35 °C to ensure full reaction of the components. Then, the reaction mixture was washed repeatedly with a sufficient quantity of DIW to effectively remove impurities and collect the solid sample. Thereafter, the collected solid samples were placed in DIW and sonicated for up to 6 h under a nitrogen-protected atmosphere to further exfoliate and disperse the samples to form a more homogeneous dispersion. Following this, the target product, namely Ti3C2 MXene nanosheets, was successfully obtained after 24 h of freeze-drying.
The LEG suspension was then mixed with Ti3C2 MXene in a 1
:
4 (v/v) ratio and ultrasonicated for a period of 3 h, resulting in the formation of the LEG@Ti3C2 MXene composite. The ultrasonic mixing step resulted in a more uniform distribution of LEG on Ti3C2 MXene nanosheets and a finer dispersion state, which lays a solid foundation for the optimization of the properties of this nanocomposite.
A mixture of 100 μL containing 20 mM EDC and 10 mM NHS was prepared and added to the Pb-Apt solution. Subsequently, 15 mg of Fc-COOH was added to the above solution, sonicated for 1 h, and then shaken for 8 h. The Fc was labeled at the end of Pb-Apt through a condensation reaction between the –COOH on Fc and the –NH2 on Pb-Apt (recorded as Pb-Apt-Fc).
As outlined in Scheme 1, the fabrication process of the duplexed-electrochemical aptasensor commenced with the modification of the ITO surface with 80 μL of LEG@Ti3C2 MXene nanocomposites (LEG@Ti3C2 MXene/ITO), followed by rinsing and drying at room temperature. Subsequently, 20 μL of 2 μM cDNA solution (a mixture of Cd-cDNA and Pb-cDNA) was drop-coated onto the electrode (cDNA/LEG@Ti3C2 MXene/ITO). Then, BSA (10 μL, 1 mM) was dropped onto the surface of the electrode and incubated for 1 h (BSA/cDNA/LEG@Ti3C2 MXene/ITO) to prevent nonspecific adsorption. Subsequently, 20 μL of 1 μM aptamer solution (a mixture of Cd-Apt-NB and Pb-Apt-Fc) was drop-costed on the electrode (Apt/BSA/cDNA/LEG@Ti3C2 MXene/ITO), and the electrode was then meticulously cleaned with MOPs. This process resulted in sensing interfaces with two types of electroactive aptamers. The electrode was rinsed with PBS buffer following each modification step and characterized using cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS).
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| Scheme 1 Schematic diagram of the duplex electrochemical aptasensor for simultaneous detection of Cd2+ and Pb2+ ions. | ||
000 rpm for 5 min and then filtered through a 0.22 μm membrane to remove any suspended matter.39 For the processing of lettuce samples, 10 g of lettuce was accurately weighed and added to 100 mL of PBS.31 Afterwards, the lettuce was crushed, filtered, and further processed using a cell disruptor. Finally, the sample was filtered through a 0.22 μm membrane to remove particulate matter.
In order to verify the presence of a single-layer structure in Ti3C2 MXene, XRD testing was conducted (Fig. S1). Following the etching of the Al layer of Ti3AlC2, it was observed that the characteristic peak of Ti3C2 MXene (002) shifted from 9.4° to a lower value of 7.1°. In addition, the characteristic peak (104) has almost disappeared, indicating a structural transformation of the material. This phenomenon is attributed to the replacement of Al elements in Ti3C2 MXene and the introduction of –OH, –O, and –F groups, thereby confirming the successful synthesis of Ti3C2 MXene.41
Fig. S2 showed the FT-IR spectra of the composite material LEG@Ti3C2 MXene, cDNA/LEG@Ti3C2 MXene, and aptamer-immobilised cDNA/LEG@Ti3C2 MXene. It can be observed that after modifying cDNA on the surface of LEG@Ti3C2 MXene, the extensive –OH groups on the material surface participate in hydrogen bonding or covalent coupling with cDNA, causing a slight shift in the broad peak at 3400 cm−1, indicating that cDNA has been successfully functionalised on LEG@Ti3C2 MXene. Subsequently, NB and Fc-modified aptamers (Cd-Apt-NB and Pb-Apt-Fc) were immobilised on cDNA/LEG@Ti3C2 MXene, and peaks at 1045 cm−1, 1108 cm−1, and 1648 cm−1, which are attributed to the stretching vibrations of the carboxyl C
O group on NB, while the peak at 3450 cm−1 corresponds to the free hydroxyl –OH group. Fc exhibited characteristic peaks below 1500 cm−1, with the 1108 cm−1 peak corresponding to the CH2X bond and the 875 cm−1 peak representing the “out-of-plane” structure of the C–H bond. These results indicated that cDNA and the aptamer successfully labelled LEG@Ti3C2 MXene.42,43
To thoroughly analyze the surface chemical bonding properties of LEG, Ti3C2 MXene, and LEG@Ti3C2 MXene composites, XPS analysis was further conducted in this study. The bonding properties of the different compositions were elaborated based on the chemical shifts of the elements by fitting the electronic binding energy curves of C 1s, N 1s, Ti 2p, O 1s, and F 1s (Fig. 1D–I). First, the elemental composition of LEG was analyzed by its core spectra (Fig. 1D). In the C 1s core spectra, the fitted peaks at 284.8 and 285.7 eV correspond to the carbon elements of LEG in the sp2 and sp3 states, respectively, while the fitted peak of C 1s at 286.5 eV indicates the presence of small amounts of oxygen atoms during the liquid stripping step as well as the DMF pretreatment of the substrate. The N 1s spectra (Fig. 1E) show a N 1s fitted peak at 399.8 eV attributed to the N
C triggered by the DMF reaction, while the peak at 401.6 eV corresponds to the graphitic nitrogen, presumed to be caused by the N-atom doping during the ultrasonic stripping process.
The results of the XPS analysis of the Ti3C2 MXene layer are displayed in Fig. 1F. The high-resolution XPS spectra in the C 1s region of the Ti3C2 MXene powder exhibited four prominent peaks at 284.8, 287.6, 291.7 and 292.2 eV, originating from Ti–C, C–C, C–O, and C
O/COO– respectively. The presence of C–O can be attributed to TiO2 and carbon atom networks, which may be produced by the oxidation reaction of Ti3C2 MXene.44 As demonstrated in Fig. 1G, the high-resolution spectra of Ti 2p of Ti3C2 MXene display two peaks at 458.2 eV and 465.5 eV, originating from the Ti–C bond within the host structure. Conversely, the peaks at 459.6, 462.3, 464.2, and 468.0 eV are attributed to the Ti–O bonds present on the surface of Ti3C2 MXene. The high-resolution spectra of the O 1s region in Fig. 1H demonstrate the presence of Ti–O, Ti–OH, C–O, and C–OH bonds. Fig. 1I clearly shows Ti–F, confirming the presence of F groups due to the etchant. Furthermore, when LEG was mixed with Ti3C2 MXene, a new C–F bond peak was identified at 689.4 eV in the high-resolution spectrum of F 1s. In combination with the aforementioned XPS analysis results, this study provides unequivocal evidence that the synthesis of LEG@Ti3C2 MXene composites has been successfully accomplished.
EIS is a sophisticated analytical instrument that provides precise information regarding alterations occurring at the electrode interface. In the high-frequency region of the EIS spectrum, the change in semicircle diameter can directly reflect the increase or decrease in interfacial charge transfer resistance (Rct). As demonstrated in Fig. 2B, the bare ITO electrode (curve a) exhibited a smaller semicircular structure with an Rct value of approximately 36 Ω. However, when the ITO electrode was modified by LEG@Ti3C2 MXene nanocomposites, its semicircle diameter (curve b) decreased significantly and the Rct value reduced to 9 Ω, a phenomenon attributed to the excellent electrical conductivity of LEG@Ti3C2 MXene nanocomposites. Following the immobilization of the Cd-cDNA and Pb-cDNA on the surface of LEG@Ti3C2 MXene/ITO electrodes, an increase in the value of Rct to 18 Ω (curve c) was observed, which can be attributed to the negatively charged phosphate backbone that exerted a hindering effect on the electron transfer process of the [Fe(CN)6]3−/4− redox probe. Following the addition of BSA and subsequent incubation, an increase in the Rct value to 180 Ω was observed (curve d), indicating that BSA successfully modified the electrode surface and hindered electron transfer. The subsequent addition of Cd-Apt-NB and Pb-Apt-Fc (curve e) resulted in hybridization to form double chains on the electrode surface, leading to an increase in the Rct value to 412 Ω. This change may be related to the repulsion between the redox probe and the negatively charged DNA phosphate backbone, as well as the blocking effect on the electrode surface. However, following the incubation of Cd2+ and Pb2+ on the modified electrode surface (curve f), a decrease in Rct value to 297 Ω was observed. This phenomenon can be attributed to the combination of Cd2+ and Pb2+ with aptamers immobilized on the electrode surface, forming Cd2+/Cd-Apt-NB and Pb2+/Pb-Apt-Fc complexes. The formation sites of these complexes exist at a distance from the electrode surface, thereby reducing the resistance. The EIS results obtained are in excellent agreement with the CV measurements, strongly demonstrating the successful development of the constructed electrochemical aptasensor.
The immobilization condition of cDNA is pivotal to optimal sensor performance. Initially, the concentration of the cDNA solution employed for immobilization was investigated, as elevated concentrations result in wastage, while low concentrations result in an excess of unspecific sites on the LEG@Ti3C2 MXene platform. This may result in a substantial background when utilizing the electrodes for the detection of the target analyte. The LEG@MXene/ITO electrodes were incubated for an equivalent duration with varying concentrations of the cDNA solution. The CV was employed to monitor the signal of each electrode. As illustrated in Fig. 3A, the peak current exhibited a pronounced increase with increasing cDNA concentration from 0.5 to 2 μM, and the modified electrode exhibited the most substantial electrochemical signal at 2 μM cDNA. This phenomenon can be attributed to the negative charge of the cDNA, which hinders the access of [Fe(CN)6]4−/3− to the electrode surface. Conversely, when the cDNA concentration was increased from 4 to 8 μM, the peak current decreased. Consequently, 2 μM was determined as the optimal concentration for cDNA immobilization. The incubation time for cDNA immobilization was also investigated, with the LEG@MXene/ITO electrodes being incubated in 2 μM of cDNA solution at different time, followed by CV detection. With the increase of incubation time, the chemical signals of the modified electrodes were rapidly enhanced and reached the maximum value within 90 min, as shown in Fig. 3B, which indicated the time required for the complete binding reaction of LEG@MXene with the inter-cDNA. Consequently, the cDNA fixation time was set at 90 min.
To ascertain the optimum concentration of aptamer that can fully react with cDNA, an increasing dose of aptamer was gradually added to the electrode surface. As demonstrated in Fig. 3C, the modified electrode exhibited the maximum electrochemical signal at a concentration of 1 μM aptamer. At a low concentration of the aptamer, it could not be fully bound to the cDNA, and the electrochemical signals were decreased significantly once the concentration of the aptamer exceeded 1 μM. This phenomenon can be attributed to the interaction between the positively charged aptamer and the negatively charged phosphate group of the cDNA, which results in an increase in background current noise and a decrease in electrochemical signals. This observation indicates that the binding affinity of aptamer and cDNA at this concentration is at its optimal level. Furthermore, the binding time between aptamer and cDNA was thoroughly investigated as illustrated in Fig. 3D. It was established that an optimal concentration of 1 μM was required for the immobilization of aptamer and that the BSA/cDNA/LEG@MXene/ITO electrodes were incubated in 1 μM aptamer solution for different durations. The experimental results demonstrated that the chemical signals of the modified electrodes climbed to the maximum value within 60 min.
The electrochemical signals of the electrodes were monitored at various intervals following the introduction of Cd2+ and Pb2+. It was found that the current of the modified electrodes showed a rapid increase with the incubation process and reached a peak at 20 min (Fig. 3E). Subsequent analysis identified this 20 min period as the optimal time for effective binding of ions to the aptamer. In addition, the ensemble sensor was examined in a variety of solutions, with pH values ranging from 6.0 to 8.5, in order to ascertain the effect of differing pH values on the aptasensors. As demonstrated in Fig. 3F, the current signals exhibited a substantial enhancement when the pH value was incrementally increased from 6.0 to 7.0; however, a notable decline was observed thereafter. This experimental phenomenon is consistent with the fact that DNA strands are deconvoluted, less stable, and more susceptible to breakage at high pH. Conversely, under acidic conditions, the presence of hydrogen ions leads to the destabilisation of hydrogen bonds, resulting in deconjugation, deformation, and even degradation of the DNA molecular structure.45 The selection of pH 7.0 as the subsequent experiments' location was informed by these considerations.
CCd2+) and with the logarithmic value of Pb2+ concentration (0.01 pM to 10 μM) (lg
CPb2+) (Fig. 4B and C). The regression equations were found to be Y = −0.011X + 0.139 (R2 = 0.998) and Y = −0.013X + 0.160 (R2 = 0.996), respectively. The LOD were measured to be as low as 0.689 pM for Cd2+ and 1.548 pM for Pb2+, with a signal-to-noise (S/N) ratio of 3.
Tables S2 and S3 presented a comparison of several electrochemical aptasensors for the detection of Cd2+ and Pb2+, encompassing pivotal parameters such as linear range, detection limit, and detection technique. Furthermore, Table S4 discussed the relevant performance parameters of other dual-signal aptasensors. A comparison of the aptasensors prepared in this paper with those reported in other references reveals that the sensors prepared in this paper demonstrate a wide linear range and lower detection limit. This finding suggested that the sensitivity of these sensors has been significantly enhanced. In comparison with the WHO and the national standard of the Ministry of Health of China, the detection levels of Cd2+ and Pb2+ were lower than the detection limits of both in drinking water, which highlights the advantages of the dual-signal sensor for simultaneous analysis of Cd2+ and Pb2+. The dual electrochemical aptasensor has been demonstrated to exhibit excellent performance for the following reasons: firstly, the LEG@Ti3C2 MXene nanocomposite possesses a substantial surface area, which can provide ample active sites and can be utilized as a substrate to enhance the loading capacity of aptamer, thereby effectively enhancing the sensitivity of the aptasensor. Secondly, the unique spatial structure of the aptamer and the strong affinity between the aptamer and the metal ions (Cd2+ and Pb2+) play a key role in facilitating signal amplification. Thirdly, the use of the labeled probe molecules (NB and Fc) combined with the DPV technique further contributes to the sensitivity improvement.
To evaluate the reproducibility of the sensor, five identical modified electrodes were prepared to fabricate the sensor using the same procedure, and five parallel measurements of its detection performance in 10 nM Cd2+ and Pb2+ were performed. The results are shown in Fig. 5B and C, with relative standard deviations (RSDs) (n = 3) of Cd2+ and Pb2+ were found to be approximately 2.29% and 1.58%, respectively, thereby indicating the excellent reproducibility of the fabricated sensors. In addition, the stability of the sensors was investigated by subjecting the electrodes to a refrigeration temperature of 4 °C for a period of ten days, and the current response was recorded daily to ascertain the ability of the modified electrodes to maintain the stability of the fabricated sensors. After ten days, the current signals of Cd2+ and Pb2+ were 87.15% and 86.63% of the original signals, respectively, and the RSD estimates of the two were 1.68% and 2.74%, respectively. These results demonstrated that the stability of the developed aptasensor was acceptable.
000 pM) of Cd2+ and Pb2+ into the samples to conduct a comprehensive recovery assessment, and the detailed outcomes are presented in Table S5. The data demonstrated that the recoveries of Cd2+ ranged from 91.413% to 104.837%, and those of Pb2+ ranged from 95.928% to 106.397%. The RSD were found to be within a reasonable range. To verify the performance of the aptasensor, we conducted consistency test using inductively coupled plasma mass spectrometry (ICP-MS), and the detection results were highly in agreement with those of the ICP-MS, indicating that the dual-signal electrochemical aptasensor exhibited excellent accuracy in resolving Cd2+ and Pb2+ in water and vegetable samples.
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