Open Access Article
Yuina Yagia,
Takahiro Kozawa
*b,
Kanako Yoshidab,
Akihiro Uehara
c,
Minoru Osada
d and
Hiroya Abe*b
aGraduate School of Engineering, The University of Osaka, Osaka 565-0871, Japan
bJoining and Welding Research Institute, The University of Osaka, Osaka 567-0047, Japan. E-mail: kozawa.takahiro.jwri@osaka-u.ac.jp; abe.hiroya.jwri@osaka-u.ac.jp
cInstitute for Radiological Science, National Institutes for Quantum Science and Technology, Chiba 263-8555, Japan
dDepartment of Materials Chemistry & Institute of Materials and Systems for Sustainability (IMaSS), Nagoya University, Aichi 464-8601, Japan
First published on 17th June 2026
Gold nanoparticles (AuNPs) underpin advances across numerous applications, yet most syntheses still rely on added chemical reductants and organic additives, constraining sustainability. Here, we report an aqueous, reductant-free route to AuNPs that leverages hydrophobic interfaces under mild conditions. When NaOH is added to aqueous HAuCl4 to reach basic conditions (pH 10–13), where [Au(OH)4]− predominates, AuNPs form spontaneously upon contact with hydrophobic fluoropolymer surfaces (e.g., PFA) without added reductants or surfactants. In contrast, almost no AuNP formation is observed on hydrophilic glass under otherwise identical conditions, indicating that interfacial rather than bulk properties govern nucleation and growth. Systematic pH tuning revealed that AuNP yield reaches a pronounced maximum at pH ≈ 12 and becomes negligible at very high alkalinity (pH 14), while particle size is tunable by varying HAuCl4 and NaOH concentrations. These results, together with the suppression of AuNP formation at high ionic strength, indicate that interfacial ion distributions, rather than bulk pH alone, play a decisive role in the reaction. A consistent interpretation is that hydrophobic interfaces promote preferential adsorption of OH−, giving rise to an electric double layer (EDL) with an ion distribution distinct from the bulk. Within this nanoscale-confined environment, ultrasmall Au(III) hydroxide-like species may form and, owing to strong size effects, undergo low-temperature transformation to yield AuNPs. These results establish interfacial EDL confinement as a basis for sustainable, reductant-free nanomaterial synthesis and suggest extension of this principle to other aqueous metal systems.
Attempts to eliminate added reductants have focused on physical methods such as laser ablation,16–18 ultrasonic irradiation,19,20 and radiation,21 which require specialized instrumentation and offer limited scalability. These constraints motivate the search for approaches that exploit inherent chemical driving forces, requiring only mild thermal energy input. Interfaces offer a compelling route: unlike bulk aqueous solutions, interfacial regions exhibit localized gradients in solute concentration, pH, and electrostatics that can enable unconventional reaction pathways.22–26 Reductant-free formation of AuNPs or gold nanoclusters has indeed been observed at microdroplet surfaces27,28 and in confined protein nanospaces,29 though the relative contributions of spatial confinement and interfacial effects remain unclear; moreover, microdroplet systems offer inherently low throughput.
This leads to a central question in interfacial chemistry: can interfacial driving forces, without relying on spatial confinement, be translated into macroscopic settings to enable practical reductant-free synthesis? Hydrophobic interfaces, which share key physicochemical attributes with microdroplet surfaces,30,31 represent an attractive yet largely unexplored option. This gap exists in part because reaction vessels are rarely treated as synthetic variables, and the surface chemistry of common labware has received little attention.32,33
Here, we demonstrate that hydrophobic polymer interfaces, including perfluoroalkoxy alkane (PFA) and polypropylene, trigger the spontaneous formation of AuNPs from basic HAuCl4 solutions (pH 10–13, adjusted with NaOH) at 25–100 °C without added reductants or surfactants, whereas hydrophilic glass remains inactive under otherwise identical conditions. Under these basic conditions, Au(III) exists predominantly as [Au(OH)4]−. The AuNP yield peaks at pH ≈ 12 and becomes negligible at pH 14, revealing a clear optimum within the basic regime.
We suggest a low-temperature, thermally assisted mechanism mediated by the electric double layer (EDL), in which [Au(OH)4]− may be locally transformed via Au(III) hydroxide-like intermediates within a nanoscale-confined interfacial environment, eventually leading to the formation of AuNPs, as elaborated in the Discussion. Collectively, these findings provide a conceptual framework for reductant-free nanomaterial synthesis and suggest that common labware surfaces may serve as an accessible platform for sustainable nanochemistry.
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1) for 1 min, followed by thorough rinsing with running water for 5 min. Second, because aqua regia can leave residual oxidizing chlorine species in PFA,34,35 a decontamination step was performed by filling the vessels with 1 M NaOH and heating at 80 °C for 3 h in an oven. After cooling, the NaOH solution was discarded, and the vessels were rinsed again with running water for 5 min. Third, the vessels were cleaned using the SC-1 method,36 a commonly employed semiconductor processing procedure. A cleaning solution of NH3, H2O2, and purified water (1
:
1
:
5 by volume) was heated to 80 °C in a water bath, and the vessels were soaked for 20 min. The solution was then discarded, and the vessels were rinsed three times with purified water, sonicated for 5 min, and dried at 100 °C for 20 min, then cooled to room temperature. For hydrophilic glass vessels, new (unused) vessels were used and only the SC-1 cleaning procedure was applied, as AuNP formation was not observed under the conditions described below.
The products were obtained as colloidal solutions. Low-magnification TEM revealed that the AuNPs were relatively uniform in size and remained well-dispersed even in the absence of surfactants (Fig. 1d). High-resolution TEM further revealed the presence of polyhedral AuNPs with distinct triangular facets (Fig. 1d, inset). The measured lattice spacing of 0.238 nm corresponds to the (111) plane of face-centered cubic (fcc) Au (SI Fig. S1a), and the selected area electron diffraction pattern confirmed the fcc crystal structure (SI Fig. S1b). The average particle size was 34.2 ± 6.3 nm, with a coefficient of variation of 18.5% (Fig. 1e). To confirm the metallic nature of the NPs, powder XRD was performed on centrifuged and dried samples. The resulting XRD pattern exhibited Bragg reflections corresponding to the (111), (200), (220), and (311) planes of fcc Au, confirming the formation of crystalline metallic AuNPs (Fig. 1f).
XRF analysis indicated a yield of approximately 28% relative to the initial gold precursor. Zeta potential measurements yielded a value of −15 mV, suggesting colloidal stability in water without surfactants, attributable to electrostatic repulsion from negatively charged particle surfaces. Colloidal stability was maintained for several days, with signs of aggregation appearing after 5 days (SI Fig. S2).
Reproducibility under standard conditions (pH 12, 80 °C, 20 h, PFA vessel) was evaluated across 27 independent syntheses. The λspr values ranged from 531 to 553 nm (average: 540 nm), and the average A400 and Aspr/A450 values were 0.09 ± 0.01 and 1.88 ± 0.06, respectively (SI Fig. S3). These results demonstrate the high reproducibility of the optical properties, yields, and particle size of the synthesized AuNPs.
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| Fig. 2 pH-dependent synthesis of AuNPs in hydrophobic PFA vessels. (a) UV-vis spectra of solutions at different pH values after reaction. (b) Photographs of the resulting solutions at each pH value. | ||
(I) Strongly acidic conditions (pH ≈ 1): in solutions adjusted to pH ≈ 1 with 100 mM HCl, no visible changes were observed after heating. The solution retained its pale-yellow color with no Tyndall effect (SI Fig. S4), indicating the absence of NP formation. The UV-vis spectrum exhibited a strong absorption band at 314 nm, characteristic of dissolved [AuCl4]−.39
(II) Weakly acidic conditions (pH 3–5): in solutions adjusted to pH 3–5 with 0–1 mM NaOH, the color intensified to a deeper yellow and a clear Tyndall effect was observed (SI Fig. S4), suggesting the formation of dispersed particulate species. The UV-vis spectra showed broad absorption below 450 nm without distinct plasmonic bands. XRD analysis of the precipitate obtained at pH 4.4 revealed diffraction patterns consistent with Au(OH)3 (SI Fig. S5), indicating that Au(OH)3 was the predominant product under these conditions. The precipitated Au(OH)3 particles were spherical with an average diameter of approximately 22 nm.
(III) Basic conditions (pH > 10): in solutions adjusted to pH > 10 with 2–10 mM NaOH, the solution turned red upon heating and a distinct Tyndall effect was observed (SI Fig. S4), confirming NP formation. The UV-vis spectra exhibited well-defined LSPR peaks in the 536–558 nm range. Within this basic regime, however, AuNP formation exhibited a clear optimum with respect to NaOH concentration rather than a monotonic increase. At pH 10–12, the A400 value increased from 0.03 to 0.09 with increasing pH, confirming an improvement in synthesis yield, while the Aspr/A450 ratio decreased from 2.04 to 1.88, suggesting the formation of smaller AuNPs. Beyond this optimum, the yield decreased markedly: at pH 12.7, A400 fell to 0.01, with only significantly smaller particles (5.4 ± 2.4 nm by TEM) detected (SI Fig. S6). At pH 14, the solution remained colorless and transparent, and AuNP formation was almost suppressed (SI Fig. S7). These results demonstrate that AuNP formation within the basic regime is non-monotonic, with an optimum around pH 12 and near-complete suppression at pH 14.
Notably, the pH remained nearly unchanged before and after the reaction under both strongly acidic (Category I) and basic (Category III) conditions. In contrast, under weakly acidic conditions (Category II), the pH decreased from 5.7 to 4.4 upon heating at 80 °C (SI Table S1), indicating proton generation during the hydrolysis of Au(III) and subsequent precipitation of Au(OH)3.
The time-dependent behavior was examined at 80 °C to assess the growth dynamics and yield of AuNPs. A400 increased with reaction time and reached a plateau after 20 h, indicating saturation of NP formation (Fig. 3c and d). Throughout the reaction, λspr remained constant, and the Aspr/A450 ratio showed little variation from 5 to 80 h (SI Table S2), indicating that particle size was established early while the number of particles continued to increase over time.
Next, the effect of initial HAuCl4 concentration on AuNP formation was investigated by varying the concentration from 0.2 to 5 mM (corresponding to final concentrations of 0.04–1 mM at pH 12). At the lowest concentration of 0.2 mM, TEM analysis revealed an average particle size of 57.9 ± 9.0 nm (SI Fig. S8), larger than that obtained under the standard conditions (34.2 nm; Fig. 1e). Aspr/A450 decreased monotonically from 1.93 to 1.64 with increasing HAuCl4 concentration, suggesting a decrease in particle size, while A400 remained nearly constant except at the lowest concentration of 0.2 mM (SI Table S2). Taken together with the temperature and reaction time dependences described above, these results indicate that temperature and reaction time are the primary factors governing yield, whereas NaOH and HAuCl4 concentrations are the primary factors controlling particle size.
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| Fig. 4 pH-dependent AuNP formation in hydrophilic glass vessels. (a) UV-vis spectra of solutions at different pH values after reaction. (b) Photographs of the resulting solutions at each pH value. | ||
The cleanliness of PFA vessels significantly impacted the reproducibility of AuNP formation (SI Fig. S9). Without cleaning, A400 remained below 0.06, and almost no AuNPs were formed. When vessels were cleaned solely by the SC-1 method to remove surface contaminants and organic residues, substantial variations were observed in both λspr and Aspr. Even after removing the residual AuNPs with aqua regia, followed by SC-1 cleaning, AuNP formation remained minimal, likely due to residual oxidizing chlorine species (Cl2/NOCl) adsorbed on the PFA surface after aqua regia treatment, which inhibit NP formation.34 To address this, a heated NaOH rinse was introduced after aqua regia cleaning to eliminate these species, followed by SC-1 cleaning. To verify the effectiveness of this protocol, AgNO3-induced AgCl precipitation tests and FTIR measurements were performed before and after each cleaning step. The absence of AgCl formation after the NaOH rinse indicated effective removal of chlorine species (SI Fig. S10), and FTIR spectra showed no detectable changes in the PFA skeletal structure, while revealing a significant decrease in surface-adsorbed organic residues after SC-1 cleaning (SI Fig. S11). Importantly, the cleaned PFA vessels exhibited no detectable redox activity: UV-vis analysis using the iodine assay revealed the absence of residual H2O2 after SC-1 cleaning (SI Fig. S12). Thus, within the sensitivity of these measurements, the cleaning protocol does not chemically modify or activate the PFA surface but rather restores a clean hydrophobic surface by removing species that would otherwise inhibit AuNP formation.
Static water contact angle measurements40 indicated that the PFA surface retains a comparable hydrophobic character after the cleaning protocol. A value of 106.8 ± 1.8° was obtained after the full cleaning protocol, which is in reasonable agreement with the reported contact angle of fluoropolymer surfaces (≈115°),41 with any minor deviation attributable to known variations in surface condition and processing history. Combined with the FTIR results showing no detectable formation of hydrophilic functional groups, these measurements reveal that the cleaning protocol removes surface contaminants without modifying the PFA interface at either the microscopic or macroscopic level.
By implementing this three-step cleaning protocol—comprising aqua regia treatment, heated NaOH rinsing, and SC-1 cleaning—a higher average A400 and reduced variation in both λspr and A400 were achieved (SI Fig. S9). These results underscore the importance of surface cleanliness for consistent and efficient AuNP synthesis at hydrophobic interfaces.
XANES analysis revealed [Au(OH)4]− as the sole Au(III) species prior to heating. Upon thermal treatment in PFA vessels, a fraction converted to metallic Au (SI Fig. S14). Parallel experiments using commercial Au(OH)3 were also performed. Although Au(OH)3 is poorly soluble in water, it dissolves in 10 mM NaOH (pH 12) owing to its amphoteric nature to regenerate [Au(OH)4]− (eqn (1)).42 Under these conditions, AuNPs formed exclusively in PFA, not in glass (SI Fig. S15). Together, these results confirm that both [Au(OH)4]− and a hydrophobic interface are required.
| Au(OH)3 + OH− → [Au(OH)4]− | (1) |
(i) Zeta potential measurements at pH ≈ 10 (SI Table S3) yield comparable values for PFA (−83.4 ± 4.2 mV) and glass (−71.4 ± 1.1 mV), yet only the hydrophobic surface supports AuNP formation. This indicates that interfacial field strength alone does not determine reactivity; rather, the origin of surface charging and the resulting EDL composition are the decisive factors.
(ii) The AuNP yield (A400) increases from pH 10 to pH 12 but drops sharply at pH 12.7, exhibiting a pronounced maximum (SI Fig. S6 and Table S2). At pH 14 (1 M NaOH), the Debye length (λD) shrinks to approximately 0.3 nm (SI Table S4), almost suppressing AuNP formation. Thus, the yield rises and then collapses as the EDL is progressively compressed, indicating that nucleation is optimized at an intermediate EDL thickness but suppressed when the diffuse layer becomes over-compressed at very high alkalinity. This behavior provides a direct experimental signature of EDL-controlled nucleation that bulk Au(III) speciation alone cannot explain.
(iii) Further support comes from ionic-strength control experiments: addition of 1 M NaCl to the pH 12 reaction medium—while maintaining pH and with Au(III) remaining predominantly as [Au(OH)4]− (SI Fig. S17)—almost suppressed AuNP formation (SI Fig. S18), mirroring the effect observed at pH 14 (1 M NaOH). Because NaCl compresses the EDL independently of pH and Au(III) speciation (λD ≈ 0.3 nm; SI Table S4), this result provides direct evidence that EDL thickness, rather than pH per se, is the critical variable governing reactivity, isolating EDL compression as the dominant factor.
Building on (i)–(iii), we outline a mechanistic interpretation in which the diffuse layer at hydrophobic interfaces serves as the reaction environment (Fig. 5), consistent with controls indicating that external reductants, substrate-derived radicals, and residual H2O2 are below detectable levels (SI Fig. S11, S12 and S16).
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| Fig. 5 Schematic illustration of a mechanistic interpretation for reductant-free AuNP formation under basic conditions at hydrophobic interfaces. | ||
The key factor distinguishing PFA from glass lies in the origin of surface charge and the resulting EDL composition. At hydrophobic PFA, the interfacial potential is dominated by specific adsorption of OH− in the Stern layer,46 which creates an OH−-enriched Stern layer and a correspondingly OH−-depleted diffuse layer, as schematically summarized in Fig. 5. In contrast, at hydrophilic glass, the negative surface charge originates from silanol deprotonation,47,48 and OH− is not specifically adsorbed (SI Fig. S19). Consequently, near-interface ion partitioning differs fundamentally, and the local OH− depletion required to promote Au(OH)3-like nucleation is unlikely to establish at glass.
At hydrophobic interfaces, the local OH− activity adjacent to the PFA surface is lower than in bulk solution due to EDL partitioning, shifting the following equilibrium toward Au(OH)3-like species within the interfacial zone (Fig. 5):
| [Au(OH)4]− ↔ Au(OH)3 + OH− | (2) |
Au(OH)3 is sparingly soluble in water yet amphoteric; therefore, Au(OH)3-like species that escape into bulk alkaline solution are expected to rapidly redissolve to [Au(OH)4]−, explaining why such intermediates remain spatially localized at the interface and do not accumulate as bulk-detectable species.
Such interfacial Au(OH)3-like species are expected to be ultrasmall, as their dimensions are constrained by the nanoscale EDL region. Due to strong size effects, ultrasmall species exhibit thermodynamic and kinetic properties distinct from bulk Au(OH)3, whose decomposition to Au(0) proceeds via Au2O3 and requires approximately 300 °C in air.49 Surface-energy contributions become dominant at reduced dimensions, lowering the activation barrier for the following transformation:
| 4Au(OH)3 → 4Au(0) + 3O2 + 6H2O | (3) |
To directly assess this size-dependent transformation, colloidal Au(OH)3 nanoparticles (average diameter: 22 nm) prepared under Category II conditions (SI Fig. S5) were subjected to hydrothermal treatment at 140 °C for 10 h. XRD confirmed metallic Au peaks alongside residual amorphous Au(OH)3, and TEM revealed irregularly shaped AuNPs coexisting with unreacted spherical Au(OH)3 particles (SI Fig. S20), demonstrating partial transformation at temperatures far below those required for bulk decomposition. The coexistence of AuNPs and Au(OH)3 phases likely reflects a broad particle-size distribution and local heterogeneity. Nevertheless, the key conclusion—that small Au(OH)3 species can undergo low-temperature transformation to Au(0) without external reductants—is strongly supported. Since the Au(OH)3-like species confined within the EDL are expected to be considerably smaller than the 22 nm Category II particles, thermolysis at relatively mild temperatures (e.g., 80 °C) becomes thermodynamically and kinetically accessible.
The most reasonable interpretation is therefore that Au(0) formation originates from the thermal transformation of interfacial Au(III) hydroxide species rather than external reductants—an interpretation that consistently accounts for the dependence on vessel material (PFA vs. glass) and ionic strength, indicating that AuNP formation is governed by a localized interfacial reaction environment rather than a homogeneous bulk-solution process. Several aspects remain unresolved, including the detailed mechanism of OH− specific adsorption, the time-dependent ion distributions within the EDL, and the nucleation and growth dynamics of interfacial Au(OH)3-like species; direct observation of such transient species in nanoscale-confined environments remains an important future challenge.
Within the parameter ranges examined here (HAuCl4 = 0.2–5 mM, NaOH = 2–50 mM), particle size can be modulated by both NaOH and HAuCl4 concentrations, albeit via distinct mechanisms. Increasing NaOH from pH 10 to 12 yields smaller particles, whereas increasing HAuCl4 concentration also shifts the size to smaller values, though the effect is less pronounced. Reaction time predominantly influences yield with little impact on size, while temperature affects both. These trends are consistent with the EDL-mediated mechanistic interpretation: NaOH largely determines ionic strength and thus EDL thickness, so increasing NaOH compresses the diffuse layer, reduces the effective interfacial reaction volume, and elevates local supersaturation—favoring more, smaller nuclei. In contrast, varying HAuCl4 has a comparatively minor effect on EDL thickness when NaOH dominates ionic strength; its influence on particle size more plausibly arises from changes in the availability of Au(III) species to the interfacial zone and the balance between nucleation and subsequent growth. Together, NaOH (EDL confinement) and HAuCl4 (Au(III) supply and nucleation–growth balance) provide complementary handles for tuning particle size under reductant-free, interfacial conditions.
Overall, productive AuNP formation requires a diffuse layer that is sufficiently developed to create an environment distinct from the bulk, yet not over-compressed by excessive ionic strength—consistent with the pronounced maximum in the pH–yield profile and the suppression observed upon adding 1 M NaCl at constant pH. This framework is qualitative and intended as a guiding picture rather than a quantitative kinetic model. Notably, this pathway is mechanistically distinct from the reductant-free AuNP formation reported by Macchione et al.,50 which occurs in homogeneous solution without surface selectivity. To provide more direct experimental evidence for the proposed mechanistic interpretation, in situ detection of transient interfacial Au(OH)3-like species, verification of O2 evolution using a sealed reactor, and direct measurement of the existence and magnitude of the interfacial electric field remain important future challenges.
The results support an EDL-mediated interfacial pathway in which preferential OH− adsorption at hydrophobic surfaces produces an interfacial environment distinct from the bulk, including a reduced effective OH− activity in the diffuse layer. This local condition can shift Au(III) chemistry from [Au(OH)4]− toward interfacially confined Au(OH)3-like species, which, owing to strong size effects, undergo low-temperature thermal transformation to metallic Au(0). The AuNP yield increases from pH 10 to 12 and decreases at higher alkalinity; at pH 14 (1 M NaOH) and upon addition of 1 M NaCl at constant pH, AuNP formation is suppressed, consistent with inhibition under EDL compression. Control experiments indicate that alternative reductive pathways involving residual H2O2 or hydroxyl radicals are not operative, and hydrothermal aging of colloidal Au(OH)3 provides direct evidence that nanoscale gold hydroxide can partially transform to Au(0) at temperatures far below bulk decomposition.
The resulting AuNPs are surfactant-free and colloidally stable for several days, with their size and yield tunable through NaOH and precursor concentrations, temperature, and reaction time. The generality of this mechanistic interpretation across chemically distinct hydrophobic surfaces points to broad applicability in other noble metal systems and offers a conceptual framework for sustainable, interface-engineered nanomaterial synthesis.
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