Open Access Article
M. A. Macchione‡
*ab,
J. E. Samaniego‡
cd,
R. Moiraghi‡ab,
N. Passarelli‡ab,
V. A. Macagno‡ab,
E. A. Coronado‡ab,
M. J. Yacaman‡e and
M. A. Pérez‡ab
aUniversidad Nacional de Córdoba, Facultad de Ciencias Químicas, Departamento de Fisicoquímica, Av. Haya de la Torre s/n, (X5000HUA) Córdoba, Argentina. E-mail: mmacchione@fcq.unc.edu.ar
bInstituto de Investigaciones en Fisicoquímica de Córdoba (INFIQC), CONICET, Av. Haya de la Torre s/n, (X5000HUA) Córdoba, Argentina
cCentro de Investigación y Estudios Avanzados del IPN unidad Querétaro, Libramiento Norponiente 2000, 76230 Real de Juriquilla, Querétaro, Mexico
dInstituto Politécnico Nacional-CICATA unidad Legaria, Calzada Legaria 694, 11500 Irrigación, Ciudad de México, Mexico
eDepartment of Physics & Astronomy, University of Texas at San Antonio, One UTSA Circle, (78249) San Antonio, Texas, USA
First published on 30th May 2018
The decomposition of gold hydroxide to give metallic gold is known to take place around 300 °C in dry environments. However, little information about the gold hydroxide stability in wet environments has been recorded. Here, we present experimental evidence which shows that aqueous/water-enriched gold(III) hydroxide colloids decompose spontaneously to form gold nanoparticles at temperature values above the freezing point of water. Based on this reaction, we developed a method to decorate silica spheres with gold nanoparticles by precipitation and decomposition of gold(III) hydroxide onto the silica surface in wet media by a simple one-pot/one-step protocol. The silica|gold nanostructures are prepared in high yield and with a low level of by-products.
The dilemma of the poor wetting on oxides is common to all metals. For the case of silver, we have recently reported a one-step/one-pot method to decorate OMPs with silver nanoparticles (AgNPs).44 In our approach, we manage to overcome the wetting problem by performing, first, the silver oxide (Ag2O) precipitation onto the OMPs in aqueous media and then, as the aqueous Ag2O decompose at room temperature to form AgNPs, we achieved the formation of AgNPs directly attached to OMP surface.45,46 As a result, OMP| AgNPs can be produced in a single synthesis step at room temperature, without drying the solution. Given that Ag2O has a good interaction with other oxides, its heterogeneous nucleation is more feasible than the heterogeneous nucleation of metallic silver. Thereby, the instability of aqueous Ag2O colloids at room temperature is the key factor of our synthetic approach. For the case of gold few information about the instability of aqueous Au(OH)3 colloids is available in literature. Besides, it is worth noting that all reports of the decoration of oxide particles using Au(OH)3 as precursor employ calcination to form metallic gold. In this context, the development of a synthetic method to obtain OMP|AuNPs with high yields simplifying the limiting factors of the pre-existing methods and avoiding calcination will have a great impact in areas as catalysis where the traditional methods are still used.
Here, we report experimental evidence which shows that aqueous/water-enriched media colloids of Au(OH)3 are unstable at temperatures above the water freezing point. Based on this behavior, we have developed a method to achieve the decoration of silica microparticles (SiO2MPs) with AuNPs. In order to obtain the optimal conditions for the synthesis of high quality OMP|AuNPs, we have explored the effect of experimental conditions (temperature, media polarity and species concentrations) on the instability of Au(OH)3 and production of AuNPs. We will refer to this synthetic approach as the Oxide Precipitation-Decomposition (OPD) method.
:
water. All the reactive mixtures were incubated in darkness at room temperature (19 < T < 24 °C). The detailed conditions of each experiment as composition of the solutions are indicated in each figure. The pH values were obtained after homogenization by using pH indicator tape.
The SiO2MPs concentration can be calculated assuming that the colloid is formed by spheres of same sizes, by using the following equation:
![]() | (1) |
50). The SiO2MPs concentration in the alcoholic suspension (10 mL) is estimated to be 1.77 × 1015 particles per liter (SiO2MPs per L). This gives an estimated concentration of 4.43 × 1014 SiO2MPs per L for the stock suspension after centrifugation and re-suspension in 40 mL. Finally, we use 0.2 mL of this stock suspension for each experiment (final volume of 20 mL) giving 4.43 × 1012 SiO2MPs per L. See SiO2MPs characterization in Section ESI-2.†
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water. Then, the reactive suspensions are incubated in darkness usually at room temperature (19 < T < 24 °C).
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10 acetone
:
water environment (final volume: 20 mL). The final concentration of NaOH is obtained gradually in three steps. By adding an aliquot from the strong base stock solution (NaOH 0.1 M) after a time lapse of 2 hours to establish the concentration in 0.1, 0.5 and 1 mM (final pH = 8.5). The beginning of the reaction time is set with the first addition of NaOH solution aliquot. This reactive suspension was kept in darkness under constant stirring during 8.5 hours of incubation in an ice bath.
• Transmission Electron Microscopy (TEM): TEM imaging was performed using JEM-JEOL 1120 and JEOL 1230 microscopes operating at 80 kV. Samples were prepared on a Formvar covered cooper grid, without any purification treatment and evaporating it in air at room temperature.
• High Resolution Transmission Electron Microscopy (HRTEM): selected experimental samples were characterized using JEOL 2010F operating at 200 kV, preparing samples on carbon covered cooper grids. Seeded grids were washed first with ethanol and then with a solution methanol
:
chloroform 50
:
50.
• Scanning Transmission Electron Microscopy (STEM): STEM imaging was performed using a Hitachi STEM-5500 operating at 30 kV. Samples were prepared on a Formvar covered cooper grid; seeded grids were washed only with ethanol.
• Atomic Resolution Scanning Transmission Electron Microscopy (ARM-STEM): a JEM-200ARMF JEOL microscope equipped with a CEOS Cs corrector on the illumination system operating at 200 kV was used; samples were seed on carbon covered cooper grids. Seeded grids were washed first with ethanol and then with a solution methanol
:
chloroform 50
:
50.
• Energy-dispersive X-ray Spectroscopy (EDS): The elemental distribution on the NSs was studied by EDS line scanning and mapping using a JEM-200ARMF JEOL microscope. The X-ray emission signals corresponding to the K lines of oxygen and silicon, and the L line of gold were used to this purpose.
• Image processing: FFT analysis was performed using the Digital Micrograph software.
• Size distribution: the size of supported AuNPs was determined from TEM images by using Image J software. For the case of spheroidal shaped particles, the criterion assumed was to regard the major dimension determined as representative value for diameter. Average values were obtained from populations ranging from 200 to 500 particles, depending on the amount of images available for each sample. Size values higher than 20 nm were considered agglomerates and they were not included in the distributions.
:
water 50
:
50 (pink line) and in aqueous media (blue line) that were incubated at room temperature. The intensity of the extinction peak obtained after 15 minutes for the acetone
:
water environment is about 26 times higher than the one obtained after 6 days in the aqueous medium. The higher extinction value indicates that the formation of AuNPs from alkaline Au(III) species is notably accelerated in acetone
:
water environments. This has a close resemblance with results obtained for silver where the silver nanoparticles formation from aqueous Ag2O decomposition is also accelerated by employing acetone
:
water environments.45
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| Fig. 1 Spectral evolution of a HAuCl4 0.1 mM and NaOH 5 mM (pH = 11–11.5) solution at room temperature. | ||
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Fig. 2 UV-Visible spectra of AuNPs produced from solutions of HAuCl4 0.1 mM and NaOH 5 mM in aqueous and 50 : 50 acetone : water media. | ||
The AuNPs formation from Au(III) alkaline solutions could be associated either with the redox reaction between [Au(OH)4]− and water or with the decomposition of aqueous Au(OH)3 colloids. Au(OH)3 has been reported to undergo thermal decomposition to produce metallic gold when calcination above 300 °C is driven in dry gaseous environments,51 in accordance to:
| 4Au(OH)3(s) → 4Au(s) + 3O2(g) + 6H2O(l) | (2) |
In aqueous media, thermodynamic calculations indicate that Au(OH)3 decomposes by the redox reaction in water.52,53 Nevertheless, there are only few experimental reports of the formation of metal gold from alkaline Au(III) solutions.54 According to this, in our experiment, either the Au(OH)3 or [Au(OH)4]− or both can be the species that lead to the AuNPs formation. In order to obtain information about the identity of the unstable species, we explored the dependence of the Au(III) stability with the base concentration (Fig. 3). The reaction spectral profiles for alkaline Au(III) solutions prepared in aqueous media and acetone
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water (50
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50) with similar strong base are shown in Fig. 3a and b, respectively. In aqueous media (Fig. 3a), the characteristic SPR peak of the AuNPs undergoes a very noticeable decrease of its extinction value as the NaOH concentration is raised. Also, the SPR peak wavelength shifts gradually to larger values with the increase of base concentration: 536 nm (5 mM), 543 nm (10 mM), and 553 nm (20 mM). Both features indicate that the nucleation of AuNPs is quenched by the increase of the NaOH concentration and, consequently, the AuNPs formed are larger in size and less in number. After the Au(OH)3 precipitation and due to the Au(III) amphoteric behavior, as the pH rises Au(OH)3 is dissolved to form [Au(OH)4]− (ESI-1†). Thus, if the instable behavior of alkaline Au(III) solutions were due to the redox reaction between [Au(OH)4]− and water, then the increase of pH should favor the AuNPs formation. Such a prediction is in plain contradiction with the experimental evidence shown in Fig. 3a and therefore, the hypothesis that AuNPs are the result of [Au(OH)4]− reduction reaction is clearly inconsistent. On the other hand, the hypothesis that AuNPs are formed by the decomposition of aqueous Au(OH)3 colloids seems to be more effective at explaining the experimental results. The evidence indicates that the AuNPs formation is more efficient at mild alkaline pH at which the Au(OH)3 is present as a colloid. Furthermore, as the pH increases the formation of the AuNPs is quenched, an effect that is consistently explained by the Au(OH)3 re-dissolution at high pH values.
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Fig. 3 UV-Visible spectra of HAuCl4 0.1 mM and different NaOH concentrations: (a) in water at 130 days. (b) in acetone : water 50 : 50 at 2 days. | ||
A similar effect on the stability of alkaline Au(III) species with the variation of pH is found for solutions prepared with acetone
:
water 50
:
50, results shown in Fig. 3b. The SPR peak decreases in intensity and is red-shifted as the NaOH concentration increases for the same reaction time. In particular, for NaOH 50 mM, the suspension exhibits a spectral profile (orange line) with small extinction values approximately constant between 400 and 800 nm, feature consistent with the dispersion of large particles. Again, the evidence shows that AuNPs nucleation is quenched by the rise in the pH, fact that is consistent with the Au(OH)3 re-dissolution to form [Au(OH)4]−. Interestingly, the formation of AuNPs is much faster in acetone
:
water 50
:
50 than it is in water as has been concluded from the analysis of Fig. 2. This feature can be consistently explained by considering the AuNPs production from Au(OH)3 decomposition since the polarity of the media of acetone
:
water environments is lower than water and, as a consequence, solvated ionic species are thermodynamically disfavor versus neutral Au(OH)3 favoring the Au(OH)3 precipitation.
The experimental evidence shown in this section demonstrate that aqueous Au(OH)3 colloids decompose at room temperature producing AuNPs. This reaction as a fact has direct application in synthesis. Indeed, the decomposition of aqueous Au(OH)3 colloids represents a safety, easy and clean method to produce free-standing AuNPs with the advantage of avoiding the use of light and high temperatures to trigger the decomposition without adding any reducing agents. As we will show in next sections, this reaction also finds application in the synthesis of hybrid NSs (SiO2MPs|AuNPs).
| [AuCl4]−(aq) + 3OH−(aq) + OMP(colloidal) → OMP|Au(OH)3(colloidal) + 4Cl−(aq) | (3) |
Since aqueous Au(OH)3 is unstable, the deposited Au(OH)3 is expected to decompose to form AuNPs:
| 4OMP|Au(OH)3(colloidal) → 4OMP|AuNPs(colloidal) + 3O2(g) + 6H2O(l) | (4) |
In this approach, an important factor is the control of the Au(OH)3 precipitation in order to favor heterogeneous nucleation onto the OMP over homogeneous nucleation minimizing the formation of free-standing AuNPs.
For the experiments, SiO2MPs synthesized by Stöber method (mean size of 227 nm, Section ESI-2†) were employed as substrate material. When the OPD method is carried on aqueous media, the reaction takes several months (see Section ESI-4†). Bright field TEM images of the OMP|AuNPs obtained are shown in Fig. 4.
The images show high contrast dots, which correspond to AuNPs, uniformly distributed onto the support material (SiO2MPs). Comparing the images of these hybrid NSs (SiO2MPs|AuNPs) with those of the substrate SiO2MPs (ESI-2 Fig. S1b†), it is evident that the incubation causes a change in the morphology of SiO2MPs, which were initially smooth spheres. It is well known that dissolution of SiO2 can take place in alkaline solutions,55 this behavior can explain the deformation of the support material after the prolonged incubation time in alkaline conditions (7 months).
TEM images show that AuNPs are surrounded by support material as they are seen inside the silica matrix. Additionally, the size values of the AuNPs obtained from TEM images (Fig. 4) present a quasi-Gaussian distribution centered on 3 nm, indicating that growth was not a predominant process. The fact that AuNPs do not grow larger, even after a prolonged reaction time (7 months), as well as the observation of the images, strongly suggests that AuNPs are immersed in the SiO2 matrix. Such a feature seems to be a consequence of an encapsulation effect caused by the chemical dissolution/re-precipitation of the silica by hydroxyl ions. Thus, these results show that it is possible to carry out the deposition of AuNPs over SiO2MPs by OPD method in aqueous media. However, the necessary prolonged incubation times are themselves a disadvantage for practical synthetic purposes as well as they get worse the quality of the NSs by the loss of the SiO2MPs spherical morphology and by favoring the encapsulation of AuNPs with silica. A way to solve this issue is to employ acetone
:
water environments in order to accelerate the AuNPs production as discussed in the previous section (Fig. 2). The study of the effect of the variation of acetone
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water ratio (see Section ESI-3†) show that when the percentage of acetone is low, 10, 25 and even 50%, Au(OH)3 precipitation/decomposition takes place quickly. Otherwise, in the case of 90% of acetone, Au(OH)3 precipitation/decomposition is delayed. Consequently, this behavior can be used to disfavor homogeneous over heterogeneous nucleation in order to achieve an effective decoration of substrate particles minimizing the formation of free-standing AuNPs. Therefore, two type of experiments were performed in parallel: the incubation of reactive mixtures in 90
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10 acetone
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water in presence of SiO2MPs and without them, this last type to be used as a control (Fig. 5a).
At room-temperature and in absence of SiO2MPs, the spectrum profile exhibits a SPR peak associated to free-standing AuNPs after 40 minutes of reaction (red line). Interestingly, this spectrum is in close resemblance with the one obtained in presence of SiO2MPs (blue line). The likeness between both spectra indicates that the AuNPs are formed mainly in the bulk of the solution (free-standing) instead of onto the SiO2MPs surface. This is probably because the Au(OH)3 precipitation/decomposition is too fast and uncontrolled under these conditions. Despite the fact that we managed to drastically reduce the incubation time for the formation of AuNPs, the use of acetone
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water mixed environments is not enough by itself in favoring the heterogeneous over the homogeneous Au(OH)3 precipitation.
Hence, two main modifications were applied to the protocol: on the one hand, the final concentration of alkali was set at a lower value than those used previously, and it was achieved by the gradual additions of aliquots of strong base solution in order to have a more controlled Au(OH)3 precipitation; on the other hand, the incubation temperature was decreased near the freezing point of water to slow down the Au(OH)3 decomposition (low-T protocol). Under these conditions, there is more time for the Au(OH)3 precipitation/dissolution cycles to occur promoting its deposition on silica since it is thermodynamically favored over its homogeneous nucleation. We also performed a control experiment where the same protocol is carried on in absence of the SiO2MPs. As expected, by lowering the temperature the AuNPs take longer to be formed and the characteristic SPR extinction appears after several hours of reaction (Fig. 5b). Although AuNPs are formed in absence of SiO2MPs (red line), the extinction in presence of SiO2MPs is notably higher (blue line), a feature pointing at different processes taking place under both conditions. These differences may indicate that silica have been decorated by AuNPs, if so, the set of experimental conditions consisting of lowering the incubation temperature, the alkali concentration and its gradual addition led to a more controlled Au(OH)3 precipitation where Au(OH)3 homogeneous precipitation is disfavored in comparison with the Au(OH)3 heterogeneous precipitation over the SiO2MPs surface. In order to confirm this interpretation samples were analyzed by electronic microscopy, results shown in the next section.
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| Fig. 6 (a and b) Bright field TEM images of the NSs obtained by the low-T protocol. (c) Size distribution of the supported AuNPs. | ||
Fig. 7a shows a STEM image of an isolated NS characterized by EDS. The NS exhibits the characteristic SiO2MP spherical shape (dark grey pattern), as well as bright zones over the surface that would correspond to gold. The element distribution over the NS was mapped by tracing the X-ray signature of O, Au and Si (ESI-5 Fig. S5†). In contrast to the homogeneous spherical distribution of O and Si (Fig. 7b and d, respectively), Au exhibits a heterogeneous pattern distribution for its EDS signature (Fig. 7c) that strongly resembles the bright pattern shown by the STEM image (Fig. 7a); a likeness that confirms the presence of gold over the surface of the SiO2MPs. The metallic nature of the deposited gold was further confirmed by HRTEM. Fig. 8a shows the HRTEM image of a single gold nanoparticle deposited on a SiO2 particle. It is observed that the nanoparticle has a decahedron morphology with stable 〈111〉 facets.56 The inset image in the upper right corner shows the Fast Fourier Transform (FFT), a representation of the crystalline structure in the reciprocal space. The FFT analysis gives a distance between the center point and the diffraction point ring of c.a. 4.021 nm−1, or an interplanar distance of 0.238 nm, which correspond to the diffraction of the 111 planes in the FCC structure of metallic gold (JCPDS 04-0784).57 Also, in Fig. 8b are shown an amplified field of the image (a) and the simulated structure of metallic gold 〈111〉 over-imposed, which perfectly fits the real atomic structure.
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| Fig. 7 A representative SiO2MP|AuNPs: (a) STEM image (dark field). EDS maps for: (b) K-oxygen, (c) L-gold and (d) K-silicon. | ||
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| Fig. 8 (a) HRTEM bright field image of one AuNP over SiO2MP; in set: FFT representation. (b) A magnified image of a; simulated structure of metallic gold superimposed. | ||
The quality of the SiO2MPs|AuNPs obtained can be appreciated from the TEM images in Fig. 6 and ESI-5 Fig. S4.† The images show that the AuNPs are homogeneously distributed onto the SiO2MPs surface and that the decoration degree is similar from one SiO2MP to another. Besides, it can be seen that the SiO2MPs have not been dissolved keeping their spherical shape. Furthermore, free-standing AuNPs are not observed which indicates that the homogeneous nucleation of Au(OH)3 (followed by its decomposition) represents a minimal contribution under the synthesis conditions. An excellent size control of AuNPs is also achieved; the AuNPs have a mean size of 9 nm (Fig. 6c).
Similar conclusions are obtained from the secondary electron images shown in Fig. 9. The images show that the AuNPs (brighter zones) also form structures of higher size values with globular morphology (highlighted with yellow circles), probably as a consequence of a growth process. Besides, it is important to highlight that AuNPs are deposited onto the surface of the SiO2MPs instead of immersed inside the matrix. This is also observed in HRTEM images in which the crystalline structure of AuNPs (Fig. 10) and gold cumulus on the SiO2MP (c) are shown. These images also show that the surface of the AuNPs is exposed to the medium confirming the absence of encapsulation which represents a positive aspect for further applications.
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c8ra01032c |
| ‡ The manuscript was written through contributions of all authors. All authors have given approval to the final version of the manuscript. |
| This journal is © The Royal Society of Chemistry 2018 |