3.1. Characterization of the electrode surface
Figure 2 illustrates the different fabricated electrodes through alloying and dealloying processes. Figure 2a shows the morphologies of the alloying structure of Ag-Au on the FTO substrate. Due to the thermal annealing process, semi-spherical Ag-Au nanoparticles are shaped on the FTO surface, wherein a hybrid layer containing a 25 nm silver thin film and a 5 nm gold thin film were initially deposited using the PVD system. In Fig. 2b, the Au nano-porous structures are visible after the dealloying process. The energy-dispersive X-ray spectroscopy (EDS) confirms the complete removal of silver during the dealloying process, as shown in Fig. 2c.
Figures 2d and 2e show the difference in hydrophilicity of the optimized Ag-Au electrode before and after the dealloying process, as demonstrated via the contact angle measurement. The porosity of the formed gold nanostructures directly effects on the measured contact angle, as the presence of nanopores on the surface increases the hydrophilicity of the working electrode. After dealloying, the contact angle decreased from 21.1\(^\circ\) to 10.4\(^\circ\), indicating that the surface had become more hydrophilic. This almost 50% decrease in the contact angle demonstrates improved hydrophilicity of the formed structure. Consequently, the low contact angle of the electrode surface leads to better connecting biomolecules to the electrode, enhancing the biofunctionality and detection capability of the sensor. To confirm the phases and components of the optimized electrode, XRD patterns were conducted, and the results are shown in Fig .2f. In addition, the XRD patterns of the bare FTO electrode, the bi-layer of 25 nm Ag and 5 nm Au electrode annealed at 550 oC, and the final nano-porous gold nanostructures have been shown for comparison purposes.
The XRD patterns provide evidence for the creation Ag-Au nanoparticles, and then the porous gold particles on the FTO substrate. The peaks of Au, Ag and FTO have many similar diffraction angles leading to appearance of several broadened peaks in the XRD spectrum. The crystallographic directions of various planes have also been displayed in the spectrums. The primary crystallographic orientations for the FTO substrate correspond to the (110), (101), (200), (211), (310), and (301) planes, with corresponding 2\({\theta }\) values of 26.6\(^\circ\), 33.8 \(^\circ\), 37.8 \(^\circ\), 52 \(^\circ\), and 62 \(^\circ\), respectively. We observe even stronger peaks for the gold and silver nanoparticles. The prominent peaks of Au-Ag nanoparticles are observed at 2\({\theta }\) values of 38.2\(^\circ\), 64.6\(^\circ\), and 77.6\(^\circ\) with the miller indices (hkl) of (111), (220), and (311) for the primary crystallographic orientations. After dealloying, nano-porous gold nanoparticles remain with the plane orientations of (111) and (220) at 2\({\theta }\) the angles of 37.5\(^\circ\) and 43.6\(^\circ\), respectively.
There are two important parameters in forming of porous nanostructures during the alloying and dealloying processes: the ratios of gold to silver in the PVD process and the annealing temperature in the thermal processing. Both of these parameters determine the size and porosity of the final porous nanostructures.
Figure 3 shows the FE-SEM images of fabricated gold nanostructures with different thickness ratio of Ag and Au layers after the dealloying process, at the same annealing temperature of 550 oC. The figure shows that the thickness ratio of silver to gold considerably affects the size of the dealloyed nanostructures. No observable porosity was revealed after post-dealloying in the case of 5 nm silver and 5 nm gold in Fig. 3a. Conversely, as the silver thicknesses increase to 10, 15, 20, 25, and 30 nm, a corresponding boost in the porosity of the emerged post-dealloying structure, is revealed. Nonetheless, no noticeable alteration occurs for silver dimensions of 25 nm and 30 nm. This conducts us to select the case of 25 nm silver and 5 nm gold arrangement as the best initial Ag-Au thicknesses for the alloy-dealloy process.
In continuation of Fig. 3 results, the morphological structures of various arrangements involving 10 nm gold thin film integrated with different silver thicknesses of 5, 20, and 40 nm were investigated, as shown in Fig. 3 (g-i). Again, no porosity was exhibited after dealloying in the case of the 10 nm gold thin film coupled with the 5 nm silver thin film. As observed previously, raised silver content correlates with increased porosity. Drawing from these figures’ analysis, one can infer that the thickness of initial silver substrate compared to the finial gold over-layer plays a crucial role in initiating and boosting the porosity of the structure. Simultaneously, the amount of gold dictates the ultimate dimensions of the formed nanostructure. However, the use of more than 10 nm gold thickness was generally limited due to the increased gold consumption, which posed economic inefficiency concerns.
To investigate and obtain an optimized annealing temperature for the thermal process, the morphologies and the average sizes of nanostructures after the dealloying process were measured as a function of the annealing temperature. As the temperature increases, the porosities become more apparent, and their surface distribution increases in the final structure. Despite this issue, according to the size distribution histograms, the overall size structure is similar for both temperatures of 550 and 600 oC. Therefore, the electrode with the annealing temperature of 550 oC with thicknesses of 25 nm silver and 5 nm gold was selected as the optimized electrode for further sensing investigations. In addition, further results of this investigation have been shown in Fig. S1, in the supplementary information.
3.2 Electrochemical characterization of the fabricated electrodes
In this section, the modified electrodes were subjected to electrochemical characterization via cyclic voltammetry and electrochemical impedance spectroscopy (EIS). The results for the bare FTO, the optimized Au-Ag electrode, and the optimized Au-Ag electrode after the dealloying process, were compared in Fig. 4a and b. Initially, the peak-to-peak potential of the FTO substrate was measured at 624 mV, and the maximum current was 620 µA. According to the EIS result, the FTO surface resistance was about 194 Ω. After modifying the FTO surface to the optimized Ag-Au layer (before the dealloying process), the silver peaks appear in the CV result at the potentials of 141 mV and 552 mV. In this case, the surface resistance reaches 56 Ω, indicating about 72% decrement relative to that of the bare FTO electrode.
In the next step, silver was dealloyed and the porous Au nanoparticles were produced. As shown in Fig. 4a and b, the current peak value of the modified porous gold electrode reaches 830 µA, indicating about 34% increase in the current compared to the pure FTO substrate. Although the peak current of the Ag-dealloyed electrode is about 12% less than this electrode before dealloying, the peak-to-peak potential for the dealloyed electrode is about 35% less than this electrode before the dealloying process. This indicates better reversibility of the dealloyed electrode against redox reactions relative to the same case before dealloying. In addition, the dealloyed electrode has a 235 mV peak-to-peak potential which is about 33% less than that of the bare FTO. Finally, the resistance of the modified dealloyed surface relative to the FTO surface decreased by 93%, reaching about 14Ω. In addition, the stability of the electrode was investigated in the first, 20th, 50th, and 100th cycles, and it is shown in Fig. 4c that no significant change was seen after the 50th cycle. In order to have an insight into the time of the dealloying process, we measured the open circuit potential (OCP) to evaluate the impact of nitric acid dealloying on the electrode surface. As illustrated in Fig. 4d, after approximately 10 minutes, nearly 94% of the change of OCP has taken place. When the OCP stabilizes, it indicates that the dealloying process is fully developed and all the silver has been completely removed. In our experiments, we have chosen an alloying time of approximately 15 minutes to ensure the complete removal of silver from the electrode surface.
In Fig. S2, the influence of the annealing temperature on the electrochemical response of the modified electrode at three annealing temperatures of 450, 550, and 600 ℃ has been investigated. The diameter of the semicircle in the Nyquist plot represents the charge transfer resistance (\({\text{R}}_{\text{c}\text{h}}\)). The \({\text{R}}_{\text{c}\text{h}}\)at the temperatures of 450 and 600 ℃ is higher than that of 550 ℃. The same scenario is also repeated for the peak current of the 550 ℃ sample, in the CV results.
As depicted in Fig. S3, it is apparent that the square root of the scan rate shows a clear linear relationship with the anodic peak current. This observation strongly indicates that the redox reaction involving the nano-porous gold nanostructures follow a diffusion-controlled process.
3.3 Immunosensing characterization and analytical performance
As previously mentioned in Fig. 1, the process of anchoring antibodies to the modified electrode and detecting the VEGF biomarker involves using MAA, EDC, and NHS. These compounds are utilized for immobilization on the modified electrode, facilitating the covalent attachment of antibodies to the transducer element. As shown in Fig. 5, the immunosensensing characterization has been performed by CV, EIS, and DPV measurements. At first, the CV, EIS, and DPV tests of the bare dealloyed electrode. we prepared these tests after immobilizing the antibody on the surface. The predominant covalent bonding of the VHH to the electrode surface leads to a further reduction in the anodic peak current to 717\({\mu }\text{A}\). After that, to block the empty places on the surface, we used gelatin, appearing in the increment of the electrode resistance from (56 Ω) for the antibody state to (107 Ω) after the block stage. In this case, the reduction of the current peak reads from (717 µA) to (610 µA). In the last step, VEGF antigen was placed on the surface to ensure the correct connection of all steps. As it is clear in the figure, in the last stage, which is also the antigen detection stage, the current peak in the CV diagram has decreased to (525 µA) in addition to about 31% increment of the peak-to-peak voltage compared to the state of Au porous. The EIS graph shows the resistance increment from (107 Ω) to (204 Ω), and the DPV diagram also shows the decrease in the current, which are all proofs of antigen detection by the desired immunosensor.
Also, result of the numerical values of the electrical parameters correspond to equivalent EIS circuit was used and the results of obtained parameters have been summarized in Fig. 5d. Also, the equivalent circuit for modeling the EIS result has been shown in the inset of Fig. 5b.
Figure 6 shows the calibration curve result of the VEGF determination by the fabricated sensor. In each step, to find the linear range, the difference between the resistances (\(\varDelta {\text{R}}_{\text{c}\text{t}}\)) with the state where VEGF is not present in the solution is measured. The equation of concentrations ranges from 0.1 pg/ml to 0.1 µg/ml can be expressed as ∆Rct(Ω) = 84.35CLog (VEGF) [gr/ml] + 1146.6 with a regression coefficient of 0.97. This immunosensor has a very good limit of detection of 0.1\(\)pg/ml. Also, in Fig. 6c the selectivity of our immunosensor has been demonstrated. It shows that the interference species produce currents that are lower than 20% of the VEGF signal. This finding indicates the high-level selectivity of this sensor for detecting VEGF, as it suggests minimal interference from other substances.
In Table.1, the characteristics of different biosensors for VEGF in the literature have been compared by this sensor. The findings illustrate that the nano-porous Au electrode outperforms various biosensors, especially regarding the limit of detection (LOD) and linear response range when of VEGF detection.
Table.1: Comparison of the analytical capabilities of different immunosensors documented for the detection of VEGF with the current research.
Biosensor substrate
|
Detection method
|
Linear range
|
LOD
|
Ref.
|
Au/3-MPA/EDC-NHS/VEGF-R1
|
CV
EIS
|
10–70
pg/ml
|
38
pg/ml
|
2
|
POLY (3,4-ethylene dioxythiophene) (PEDOT)/Gold Nanoparticle (Au NP) Composites
|
EIS
|
1–20
pg/ml
|
0.5
pg/ml
|
29
|
PdPtMo CME NPs
|
EIS
|
10–106
pg/ml
|
8.2
pg/ml
|
30
|
RGO/Au NPs/11MUA/Antibody/VEGF/HRP
(Sandwich type)
|
CV
SWV
EIS
|
2-20000
ng/ml
|
6
fg/ml
|
31
|
cellulose paper
|
fluorescence control (FApt)
|
100–5000
ng/ml
|
137
ng/ml
|
32
|
Au nano porous/MAA/EDC-NHS/VHH/Gelatin/VEGF
|
CV
EIS
|
\({10}^{-4}{-10}^{2}\)
ng/ml
|
0.1
pg/ml
|
This work
|