Jing
Xu
a,
Yujin
Li
ab,
Futing
Wang
b,
Xinqi
Luo
a,
Wei
Zhang
f,
Yifan
Lyu
b,
Hongfen
Yang
e,
Ren
Cai
*b and
Weihong
Tan
bcd
aCollege of Chemistry and Chemical Engineering, Xinyang Normal University, Xinyang 464000, China
bMolecular Science and Biomedicine Laboratory, State Key Laboratory for Chemo/Bio-Sensing and Chemometrics, College of Material Science and Engineering, College of Chemistry and Chemical Engineering, College of Biology, Hunan University, Changsha, Hunan 410082, China. E-mail: cairen@hnu.edu.cn
cThe Cancer Hospital of the University of Chinese Academy of Sciences (Zhejiang Cancer Hospital), Hangzhou Institute of Medicine, Chinese Academy of Sciences, Hangzhou, Zhejiang 310022, China
dInstitute of Molecular Medicine, Renji Hospital, Shanghai Jiao Tong University School of Medicine, College of Chemistry and Chemical Engineering, Shanghai Jiao Tong University, Shanghai 200240, China
eHunan Key Laboratory of Typical Environmental Pollution and Health Hazards, School of Public Health, Hengyang Medical School, University of South China, Hengyang 421001, China
fCollege of Life Science, Xinyang Normal University, Dabie Mountain Laboratory, Xinyang 464000, China
First published on 11th October 2024
A bidirectional self-powered biosensor is constructed for the quasi-simultaneous detection of Pb2+ and Hg2+ based on MoS2@CuS heterostructures as an accelerator and hybridization chain reaction (HCR) as a signal amplification strategy. MoS2@CuS heterostructures significantly facilitate electron transfer between glucose and bioelectrodes, thereby greatly improving the detection signal of self-powered biosensors. This novel biosensor employs the unique sequences of DNAzymes to isolate Pb2+ and Hg2+ by the cleavage effect and thymine (T)–Hg2+–thymine (T) structures, respectively. In the process, Pb2+ cuts the sequence of DNAzyme at the bioanode to trigger glucose oxidation to monitor Pb2+. The as-formed T–Hg2+–T structures activate HCR to reduce [Ru(NH3)6]3+ to detect Hg2+ at the biocathode. It is noteworthy that this biosensor not only realizes Pb2+ or Hg2+ detection in a single-electrode, respectively, but also can quasi-simultaneously detect both Pb2+ and Hg2+ in the bioanode and the biocathode. The novel self-powered biosensor identifies Pb2+ in the range of 106 fM to 10 fM with a limit of detection (LOD) of 3.1 fM and Hg2+ in the range of 106 fM to 1 fM with an LOD of 0.33 fM.
Compared with the above methods, self-powered biosensors are widely used in the detection of biomolecules. In addition to eliminating the need for external power, these sensors exhibit strong anti-interference ability, ultra-sensitive detection capability, and highly identifiable specificity.17–21 However, there has been no report of self-powered biosensors with the bidirectional detection to monitor heavy metal ions. The major reason is the difficulty in forming double bioelectrodes to simultaneously achieve linear detection.22–24 Therefore, a bidirectional self-powered biosensor toward multiple heavy metal ions detection is urgently needed.
This work reports a bidirectional self-powered biosensor for the quasi-simultaneous detection of Pb2+ and Hg2+ based on MoS2@CuS heterostructures as a co-accelerator and a hybridization chain reaction (HCR) as a signal amplification strategy (Scheme 1). Unique sequences of DNAzymes isolate Pb2+ and Hg2+ by the cleavage effect and thymine (T)–Hg2+–thymine (T) structures, respectively.25–29 In the process, Pb2+ cuts the sequence of the DNAzyme at the bioanode to trigger glucose oxidation to monitor Pb2+. The as-formed T–Hg2+–T structures activate HCR to reduce [Ru(NH3)6]3+ to detect Hg2+ at the biocathode. As a result, this biosensor not only monitors Pb2+ or Hg2+ through the current changes caused by the oxidation–reduction reactions in a single-electrode, respectively, but also could quasi-simultaneously detect both Pb2+ and Hg2+ by observing the open circuit voltage (Eocv) in the bioanode and the biocathode. The bidirectional biosensor also exhibits considerable practicability for detecting Pb2+ and Hg2+ in tap water.
Scheme 1 (a) The synthetic process of MoS2@CuS heterostructures. (b and c) The detection process of Pb2+ and Hg2+ of the bidirectional self-powered biosensor. |
Fig. 1 Characterization of MoS2@CuS heterostructures: (a) TEM image and SAED (insert); (b) XRD. (c) TEM image and (d) EDX images of AuNPs/MoS2@CuS heterostructures. |
The assembly process of the bioanode and biocathode was explored by cyclic voltammetry (CV) and differential pulse voltammetry (DPV). Monitoring the maximum current value, the optimal recognition and cleavage time of Pb2+ on the DNAzyme was 60 min (Fig. 2a). After DNAzyme was cut by Pb2+, it was split into two sequences of single strand DNAs: S1 and S2, leaving as-split S2 on the surface of AuNPs/MoS2@CuS/CP by Au–S bonding. When S3-GOD is added, the as-split S2 hybridizes with S3-GOD by complementary base pairing to form the bioanode. The optimal hybridization time between S2 and S3-GOD is 50 min (Fig. 2b). In the biocathode, the optimal incubation time among Hg2+, S5, and S4 is 30 min to form S5–Hg2+/S4/AuNPs/MoS2@CuS/CP by the T–Hg2+–T structure (Fig. 2c). Finally, the as-formed T–Hg2+–T structure further combines with H1 and H2 from the HCR process to generate a multi-duplex structure of H1, H2, and S5 to form H1, H2/S5–Hg2+/S4/AuNPs/MoS2@CuS/CP.
Next, [Ru(NH3)6]3+ inserts into the multi-duplex structure of H1, H2, and S5 on the surface of H1, H2/S5–Hg2+/S4/AuNPs/MoS2@CuS/CP (Fig. 2d) with optimal concentration of 500 μM [Ru(NH3)6]3+. These assembly processes of the bioanode and biocathode were further verified by gel electrophoresis (Fig. 2e). Line M represents molecular weight standards. For the bioanode, a fading, shallow band with low molecular weight appears when Pb2+ (lane 2) is incubated with DNAzyme (lane 1). After S3-GOD is added, S3-GOD hybridizes with as-split S2 to form many new bright bands (lane 3). For the biocathode, there is no visible band for S4 (lane 4) or S4 + S5 (lane 5), respectively. When the T–Hg2+–T (i.e., S4–Hg2+–S5) structure is formed, a higher bright band (lane 6) is observed. Finally, when the T–Hg2+–T structure triggers the HCR reaction, a new band is observed (lane 7). These results are consistent with circular dichroic chromatography (Fig. S7†). In the sensing mechanism, the Pb2+ could cleave the RNA sites and change the DNAzyme structure; the thymine–thymine mismatch base pair (T–T, H1–H2) can capture the Hg2+ to form a stable neutral T–Hg2+–T base pair.
Electrochemical impedance spectroscopy (EIS) was used to study the preparation process of the bioanode (Fig. 3a). The resistance (Ret) value of CP (curve A) is higher than that of AuNPs/MoS2@CuS/CP (curve B), confirming the good electrical conductivity of AuNPs/MoS2@CuS. After DNAzyme, Pb2+, and S3-GOD are sequentially incubated with AuNPs/MoS2@CuS/CP, the Ret increases from 14 Ω to 30 Ω (Fig. 3a). For the biocathode (Fig. 3b), H1, H2/S5–Hg2+/S4/AuNPs/MoS2@CuS/CP shows the highest Ret after S4, S5 and Hg2+, and H1, H2 are modified the biocathode. In addition, the ζ-potential measurements confirmed the successful assembly of the bioanode and biocathode (Fig. S8†). CV and linear scanning voltammetry (LSV) were performed to verify the catalytic reaction of GOD on the bioanode. In PBS with 5 mM glucose, a distinct oxidation peak at −0.48 V is observed (blue line), which corresponds to the splitting of DNAzyme to S1 and S2 by Pb2+, and the as-split S2 triggers the oxidation of glucose (Fig. 3c and d). The feasibility of the biocathode for Hg2+ detection was investigated by DPV. In PBS with 500 μM [Ru(NH3)6]3+, as-adsorbed [Ru(NH3)6]3+ acquires electrons and is reduced to [Ru(NH3)6]2+ at the biocathode. When AuNPs/MoS2@CuS (black line), S4 (blue line), S5, Hg2+ (green line), and H1, H2 (red line) are successively coated on the CP surface, H1, H2/S5–Hg2+/S4/AuNPs/MoS2@CuS/CP exhibits the largest peak current value (Fig. 3e). Finally, the current of DPV was increased when the biocathode combined with the HCR strategy (Fig. S9†), which confirmed the signal amplification effect of HCR. These results prove the efficient signal amplification strategy from HCR for the biocathode.
In Fig. 4a and b, there is a linear relationship between the peak current with increasing scan rate in the range of 60 to 200 mV s−1 (peak potential difference ≤ −20 mV), which proves that the as-prepared bioanode and biocathode exhibit accurate identification ability.34,35 Here, one biosensor was constructed based AuNPs/CP as the bioanode and the biocathode; the other one was fabricated based on AuNPs/MoS2@CuS/CP as the bioanode and the biocathode. The Eocv of the biosensor based on AuNPs/MoS2@CuS/CP is about 0.58 V, which is 0.13 V higher than that of the biosensor based on AuNPs/CP (Fig. 4c). Similarly, the maximum power output of the biosensors based on AuNPs/MoS2@CuS/CP and AuNPs/CP is 49.5 μW cm−2 and 33.2 μW cm−2, respectively (Fig. 4d), which proves high-efficiency conduction of MoS2@CuS heterostructures.
For the single detection of Pb2+, the peak intensity of glucose oxidation at −0.48 V increases with increasing Pb2+ concentration under optimal conditions in a CV test at the bioanode (Fig. S10†). Moreover, there is a good linear relationship between the logarithm of Pb2+ concentration and current intensity in the range of 10 fM ∼1 nM. The equation is: I = 0.01 × logCPb2+ + 0.20 (correlation coefficient, R2 = 0.995), and the detection of limit (LOD) is calculated to be 3.1 fM (S/N = 3). Analogously, the current response at −0.18 V is attributed to the reduction of [Ru(NH3)6]3+ in the DPV test at the biocathode, which gradually increases with increasing Hg2+ concentration (Fig. S11†). A linear correlation between the logarithm of Hg2+ concentration and current intensity in the range of 1 fM to 1 nM was fitted by the regression equation: I = 0.1 × logCHg2+ + 2.4 (R2 = 0.995), and LOD is calculated to be 0.32 pM (S/N = 3).
For the bidirectional detection of Pb2+ and Hg2+, Eocv of the novel biosensors was investigated at the double electrodes (Fig. 5). For instance, Hg2+ concentration is determined to be 1 nM at the biocathode in a tap water sample (Fig. 5a and b). A good linear relationship between Eocv and the logarithm of Pb2+ concentration is calculated: Eocv = 0.078 logCPb2+ + 1.21 (R2 = 0.994) with the LOD of 3.1 fM (S/N = 3) in the range of 10 fM to 106 fM. Here, the Eocv increases with the increment of Pb2+ concentration at the bioanode. In another example, Pb2+ concentration is determined to be 1 nM at the bioanode in the same tap water sample (Fig. 5c and d). There is a linear relationship between Eocv and the logarithm of Hg2+ concentration in the range of 1 fM to 106 fM: Eocv = 0.083 × logCHg2+ + 1.34 (R2 = 0.995), and the LOD is calculated to be 0.33 fM (S/N = 3). Here, the Eocv increases with the increment of Hg2+ concentration at the biocathode. Compared with previously reported sensors (Tables S2 and S3†), the bidirectional self-powered biosensor shows wider detection ranges and lower LODs for Pb2+ and Hg2+ detection. In order to further visualize the on-site detection of Pb2+ and Hg2+, our capacitor amplification strategy was explored by smart Bluetooth data transfer with a smartphone for real-time read-out of test results (Fig. S12 and see Movie S1†).36–38 In the test process, the mobile phone reads out the instantaneous current when different concentrations of Pb2+ and Hg2+ are in an unknown water sample, furthering realizing on-site and real-time detection (Fig. S13 and S14†).
The signal responses of the self-powered biosensor toward Pb2+ and Hg2+ detection remained at 83.5% and 82.1% of original signal after the biosensors were stored at 4 °C for 15 days, further confirming the long-time stability (Fig. S15†). The recyclability of one as-designed biosensor was tested by analyzing different concentrations of Pb2+ and Hg2+. All test results maintained within 5% of the error, which confirmed good recyclability for the biosensor (Fig. S16†). To confirm the specificity, there was no Eocv signal when six possible interferences, i.e., Na+, K+, Mg2+, Cu2+, Co2+, and blank water sample, were detected by the as-designed biosensor. The solution with Pb2+ or Hg2+ showed significantly high Eocv, thus verifying the good specificity of the bidirectional biosensor (Fig. S17†). In addition, the relative standard deviations (RSDs) were measured to be ≤5% in five parallel experiments, indicating the good repeatability of the novel biosensor (Fig. 5e and f). To further test the practical application, Pb2+ and Hg2+ with the concentrations of 1, 10, 50, and 100 nM in tap water and lake water were prepared to perform a labelled recovery experiment. The RSDs values were calculated to be the range from 3.7% to 5.3% for Pb2+ and 2.1% to 5.9% for Hg2+; and the recovery rates were in the range from 96.4% to 105.0% for Pb2+ and 97.0% to 104.8% for Hg2+ (Tables S4 and S5†). These results demonstrate that the bidirectional self-powered biosensor possesses good selectivity, stability, and reproducibility, and could be used for practical sample detection.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4sc04404e |
This journal is © The Royal Society of Chemistry 2024 |