Open Access Article
Setia
Budi
*a,
Annisa
Auliya
a and
Hilman
Syafei
b
aDepartment of Chemistry, Faculty of Mathematics and Natural Sciences, Universitas Negeri Jakarta, Jl. Rawamangun Muka, Jakarta 13220, Indonesia. E-mail: setiabudi@unj.ac.id
bThe Center for Science Innovation, Arva Building, Jl. RP. Soeroso, Jakarta Pusat 10350, Indonesia
First published on 21st October 2025
Gold nanoparticles (AuNPs) exhibit unique catalytic, electronic, and optical properties, making them highly suitable for various applications, particularly in catalysis. This study explores the synthesis of AuNPs on fluorine-doped tin oxide substrates using a square-wave pulse deposition technique, with deposition time as the primary variable influencing nanoparticles growth. The synthesized AuNPs were systematically characterized using field emission scanning electron microscopy, energy dispersive X-ray spectroscopy, and X-ray diffraction techniques. The electrocatalytic performance of the synthesized AuNPs was evaluated through electrochemical impedance spectroscopy and cyclic voltammetry in an alkaline medium. The results revealed that longer deposition duration led to nanoparticle increased coverage, improved charge transfer kinetics, and enhanced catalytic activity. Notably, AuNPs50 deposited for 50 minutes exhibited the the lowest charge transfer resistance and the highest electrochemical surface area, resulting in the highest current density during ethanol electrooxidation. These findings demonstrate the enhanced catalytic performance of the electrodeposited AuNPs for ethanol oxidation, achieved without the use of surfactants or additives.
Contemporary approaches for the synthesizing AuNPs with controlled morphologies often involve the use of additives,16 surfactants,17 or templates.18 However, surfactants and directing agents can introduce impurities, while template-assisted methods typically require post-synthetic treatments that may compromise the structural integrity of the nanomaterials.19,20 In contrast, electrodeposition offers a rapid, straightforward,21 and effective approach for synthesizing nanomaterials with well-defined structures,22,23 without the need for additives, surfactants, or templates.24,25 Key parameters in the electrodeposition process, such as applied voltage, pH, electrolyte concentration, and deposition duration, can be systematically adjusted to influence surface coverage, particle morphology, and size.26–28 These structural characteristics play a critical role in determining the electrocatalytic performance of AuNPs.
In this study, the square-wave pulse deposition technique was employed due to its ability to precisely control the deposition process, specifically nucleation and growth, by alternating between two distinct potentials over a defined time interval. This approach is essential for producing controlled-size nanoparticles from an additive-free solution, which can significantly influence the performance of the ethanol electrooxidation reaction (EOR). The deposition time was used as the primary parameter to regulate AuNPs via this technique. By minimizing excessive growth, the method aims to preserve the catalytic activity of the nanoparticles. The synthesized AuNPs were subsequently evaluated for their catalytic performance in ethanol oxidation in alkaline solutions.
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| Fig. 1 Electrodeposition schematic of the AuNPs using square-wave pulse deposition conducted by varying deposition duration. | ||
The electrocatalytic activity of AuNPs toward ethanol oxidation of ethanol was evaluated using cyclic voltammetry (CV) technique within a potential range of −0.75 to 0.75 V at a scan rate of 25 mV s−1. The measurements were performed using an ER466 potentiostat in an electrolyte solution containing 1 M ethanol and 0.1 M NaOH.
The observed trend in nanoparticles morphology can be attributed to the dynamic interplay between competing nucleation and growth mechanisms during the deposition process. Nucleation typically initiates at high-energy surface sites, such as defects, cavities, and grain boundaries, leading to the formation of dispersed particles. As the deposition duration increases, these high-energy sites become saturated, promoting enhanced particle growth and resulting in larger and denser nanoparticles. The agglomeration observed at extended deposition durations, particularly at 50 minutes, suggests the onset secondary nucleation occurring on pre-existing particles. This phenomenon disrupts the uniform growth of particles across the substrate and marks a transition from surface-limited nucleation to particle–particle interactions.
Energy-dispersive X-ray spectroscopy (EDX) was employed to confirm the presence of gold on the fluorine-doped tin oxide (FTO) substrate. The EDX spectrum revealed characteristic peaks corresponding to gold at approximately 2–2.5 keV and 9.5–10 keV, as shown in Fig. 3. Additionally, the EDX elemental mapping confirmed the spatial distribution of Au across the sample surface. The presence of additional peaks is attributed to the elements fluorine (F), tin (Sn), and oxygen (O) originating from the substrate. To further investigate the formation of metallic phase of Au, the samples were analyzed using X-ray diffractometer (XRD). The complete XRD patterns for AuNPs deposited at 1, 5, 10, and 50 minutes are presented in Fig. S1. To better visualize the peaks associated with AuNPs, a selected region of the patterns, excluding the 2θ range from 46° to 63°, is shown in Fig. 4. From these patterns, four distinct diffraction peaks were observed at 2θ values of 38.11°, 44.36°, 64.44°, and 77.68°, corresponding to the (111), (200), (220), and (311) crystallographic planes of face-centered cubic Au, respectively. These results are consistent with standard reference data for Au (Crystallography Open Database No 96-900-8464). The (111) peak at 38.11°, although partially overlapping with the FTO substrate peak at 37.85°, became increasingly prominent with longer deposition times due to the enhanced intensity of Au diffraction. This increase in peak intensity correlates positively with extended deposition durations, which promote the growth of larger Au grains. This observation is further supported by the increase in crystallite size (Table 1), calculated from the (111) peak using the Scherrer equation. The trend aligns with the SEM micrographs (Fig. 2), indicating a positive correlation between deposition time and AuNPs particle size. These findings confirm the successful synthesis of metallic Au, where the presence of larger particles contributes to the intensified diffraction signals observed in samples subjected to longer deposition durations.
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| Fig. 3 A representative of EDX spectrum (a) and an EDX elemental mapping of the electrodeposited AuNPs on FTO-coated glass substrate (b). The inset is distribution of Au element over the substrate. | ||
| Electrocatalyst | Crystallite size (nm) | R ct (Ω) | ECSA (cm2) |
|---|---|---|---|
| AuNPs1 | 21.29 | 25.99 | 3.11 |
| AuNPs5 | 32.54 | 21.38 | 6.87 |
| AuNPs10 | 33.04 | 17.69 | 8.30 |
| AuNPs50 | 52.38 | 15.31 | 9.60 |
Nyquist plots obtained from electrochemical impedance spectroscopy (EIS) measurements (Fig. 5) demonstrate a pronounced decrease in charge transfer resistance (Rct) with increasing Au deposition duration. The equivalent circuit used to fit the data is illustrated in the inset of Fig. 5a, where R1 represents the solution resistance (Rs) and R2 corresponds to the Rct. In the Nyquist plot, the semicircular region reflects the charge transfer process, while the linear region at lower frequencies is indicative of mass transport limitations. The analysis focuses primarily on Rct values, which are critical for evaluating the charge transfer kinetics of the catalytic system. Among the samples, the AuNPs1 exhibits the highest Rct, attributed to the limited presence of irregularly shaped particles that provide insufficient surface area for efficient electron transfer. As the deposition duration increases, the Rct progressively decreases, with AuNPs50 showing the lowest Rct value, suggesting enhanced electron transfer kinetics. This reduction in Rct is ascribed to the intrinsic conductivity of gold and the increased particle density grown on the FTO substrate. The greater number of deposited AuNPs significantly enlarges the electrochemically active surface area, thereby facilitating improved charge transfer and lowering the overall resistance. To further confirm this observation, the electrochemical active surface area (ECSA) was determined from the EIS data by evaluating the double-layer capacitance (Cdl) in the non-faradaic region. As shown in Table 1, ECSA values increase with longer deposition durations, indicating a greater number of active sites available for electrochemical reactions and, consequently, enhanced catalytic activity of the catalyst.
The electrocatalytic performance of AuNPs for the oxidation of ethanol was evaluated using cyclic voltammetry (CV) technique in an alkaline electrolyte comprising 0.1 M sodium hydroxide (NaOH) and 1 M ethanol. Fig. 6 presents the cyclic voltammograms of AuNPs synthesized at various deposition durations. During the anodic scan, a prominent peak at approximately 0.25 V is attributed to the oxidation of ethanol on the gold surface. In the reverse scan, a peak observed at 0.09 V corresponds to the oxidation of adsorbed carbon monoxide (CO) species, which are well-established intermediates in the ethanol oxidation pathway.29 Control experiments conducted in NaOH electrolyte without ethanol demonstrated negligible anodic activity, confirming that the observed peaks are directly linked to the oxidation of ethanol. Additional minor peaks observed at 0.4 V, along with reductions features at −0.1 V and 0.15 V in NaOH-only system, are indicative of oxide formation and oxide stripping, respectively.14 Furthermore, CV measurements of bare FTO substrates yielded in flat voltammograms, suggesting the absence of significant electrochemical activity. This observation further confirms the catalytic role of AuNPs in facilitating ethanol oxidation.
The catalytic activity, quantified by the anodic peak current density, exhibited a notable increase with longer deposition times, yielding values of 0.58 mA cm−2, 24 mA cm−2, 259 mA cm−2, and 6.38 mA cm−2 for the samples designated as AuNPs1, AuNPs5, AuNPs10, and AuNPs50, respectively. This enhancement is attributed to the increased number of nanoparticles and improved charge transfer efficiency resulting from higher density particles achieved during extended deposition durations. The electrochemical impedance analysis supports this observation, showing a reduction in charge transfer resistance (Rct) with prolonged deposition times, which facilitates more efficient electron transfer and accelerates the rate of the catalytic reaction.30–32 Additionally, the Tafel slope (Fig. 7) values decreased from 453 mV dec−1 for AuNPs1 to 232 mV dec−1 for AuNPs50, further indicating enhanced electron transfer kinetics with prolonged deposition. As summarized in Table 2, the ratio of backward to forward current density (jb/jf) also declined with increasing deposition durations, suggesting enhanced catalyst stability and a greater resistance to poisoning by carbon monoxide intermediates. These results collectively demonstrate that increased particle size and density lead to improved electrocatalytic performance and long-term stability of the AuNPs.
| Electrocatalyst | E onset (V vs. Ag/AgCl) | j (mA cm−2) | j b/jf | Tafel slope (mV dec−1) |
|---|---|---|---|---|
| AuNPs1 | −0.32 | 0.58 | 0.49 | 453 |
| AuNPs5 | −0.23 | 1.24 | 0.40 | 375 |
| AuNPs10 | −0.43 | 2.59 | 0.33 | 297 |
| AuNPs50 | −0.13 | 6.38 | 0.29 | 232 |
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