Xiaojing Yuab,
Tomohiro Shirakib,
Shengchun Yanga,
Bingjun Dinga and
Naotoshi Nakashima*bc
aSchool of Science, Key Laboratory of Shaanxi for Advanced Materials and Mesoscopic Physics, State Key Laboratory for Mechanical Behavior of Materials, Xi’an Jiaotong University, Xi’an 710049, ShaanXi, People’s Republic of China
bDepartment of Applied Chemistry, Graduate School of Engineering, Kyushu University, 744 Motooka, Nishi-ku, Fukuoka 819-0395, Japan. E-mail: nakashima-tcm@mail.cstm.kyushu-u.ac.jp
cInternational Institute for Carbon-Neutral Energy Research (WPI-I2CNER), Kyushu University, 744 Motooka, Nishi-ku, Fukuoka 819-0395, Japan
First published on 29th September 2015
We describe a facile method for preparing porous gold nanoparticle (Au-NP)/2H-form MoS2 nanocomposites. The Au-NPs were formed by redox reactions between 2-dimensional MoS2 nanoflakes with a 2H-form crystal structure and tetrachloroauric acid (HAuCl4) in a water/ethanol mixture without adding any additional reducing agents. The structures of the Au-NP/MoS2 nanocomposites were influenced by the molar ratio of the Au ion precursor and MoS2, as well as the volume ratio of water and ethanol in the reaction mixture. Ethanol allowed the 2H-MoS2 nanoflakes to maintain their original morphologies after the reaction to serve as the support framework, meanwhile the Au-NPs worked as a junction to construct a 3-dimensional (3D) nanoporous structure. The obtained porous nanocomposites worked as a material for surface enhanced Raman spectroscopy (SERS) due to the formation of many nanoholes with so-called “hot-spots” based on the assembled Au-NPs.
MoS2 exhibits a unique 2D S–Mo–S structure in which the molybdenum atom layer is sandwiched between two close-packed sulfide atom layers through strong covalent bonding.13 The outer-layered S atoms can joint different metal or oxide nanoparticles which can expand the use of MoS2-based materials for many applications.14–18 Recently, noble-metal decorated MoS2 has been extensively studied since a possible synergistic effect between the noble metals and MoS2 might induce a novel function.19–21 Huang et al. reported a general method to reduce Pt, Au, Ag, and Pd ions to form nanoparticles on the MoS2 nanosheets using an ascorbic acid aqueous solution and a carboxymethylated cellulose (CMC) aqueous solution as the reducing agent and stabilizer,22 respectively. Huang et al. reported that the Pd, Pt and Ag NPs were prepared by using a reducing agent followed by epitaxial growth on the 2-D MoS2 nanosheets.23 The Berry group used both chemical reduction and microwave irradiation to anchor Au-NPs on the MoS2 ultrathin nanosheets.24 A microwave-assisted hydrothermal method was also reported as an effective approach to decorate Au-NPs on MoS2 nanosheets.25,26 Without using such reducing agents or complicated preparation methods, Au-NPs are spontaneously formed and anchored on the MoS2 nanosheets.27 However, up to now, many studies have focused on growing Au-NPs on 1T-MoS2 due to their metallic properties and the structure of the Au-NP-decorated MoS2 nanocomposites shows a sheet-like 2-dimensional structure.
In this paper, we firstly construct porous Au-NP/2H-MoS2 nanocomposites based on a facile and green in situ growing method, and then apply them as a material for a surface-enhanced Raman spectroscopy (SERS) substrate. We also describe a finding that the morphology of the Au-NP/MoS2 nanocomposites could be changed by altering the concentration of HAuCl4 and the volume ratio of ethanol/water. The synthesized Au-NP/MoS2 substrates exhibited an efficient SERS enhancement based on the formation of porous structures of the compound and assembled Au-NPs.
STEM observations were conducted to investigate the morphologies of the prepared composites. As a control sample, commercially available pristine MoS2 nanoflakes were used. Fig. 1A shows the control sample prepared after 1 h of sonication, in which well-dispersed MoS2 fragments were observed. On adding HAuCl4 to the solution with a molar ratio of Au3+:
MoS2 = 0.5
:
1, Au-NPs grew only at the edge of the MoS2 (Fig. 1B). When the molar ratio of Au3+
:
MoS2 was increased to 1
:
1, Au-NPs with diameters of ∼16 nm were decorated on the surfaces of the MoS2 as shown in Fig. 1C. The composites were well-dispersed in the solution, and the color of the solution did not change until the molar ratio of Au3+ and MoS2 reached 5
:
1 as shown in the insert of Fig. 2. When the molar ratio of Au3+
:
MoS2 > 5
:
1, the color of the solution turned to wine red, suggesting that the Au-NPs grew larger. From the SEM images shown in Fig. 1D and E, it was found that both small (2–5 nm) and large (>20 nm) Au-NPs grew on the surfaces of the MoS2. The average size of the large Au-NPs on the Au-NP/MoS2 nanocomposites increased from 16.3 nm to 51.1 nm when the molar ratio changed from 1
:
1 to 10
:
1 (Fig. S1†). Compared to a report that describes the destroying of MoS2 at high HAuCl4 ratios through a spontaneous redox reaction,25 in our experiments the MoS2 nanoflakes maintained their flake shape even at the high ratios of Au ions.
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Fig. 2 (A) UV/vis spectra of the commercial pristine MoS2 nanoflakes and specified Au-NP/MoS2 nanocomposites, and photographs of the samples. (B) UV/vis spectra in the range of 300–800 nm. |
The optical properties of the prepared nanocomposites were examined using UV/vis spectroscopy, and the results are shown in Fig. 2, in which two peaks were observed at 606 nm and 665 nm, indicating that the materials contain pristine MoS2 crystals with the 2H crystal structure.28 No obvious difference was observed between the spectra of the pristine MoS2 and the nanocomposites with molar ratios of Au3+ and MoS2 lower than 5:
1. When the amount of the Au3+ precursor was increased to 5
:
1, a new peak around 545 nm appeared, indicating the formation of Au-NPs that show surface plasmon resonance (SPR) spectra. Compared to the composite with a 5
:
1 molar ratio, the peak wavelength of the composite with the 10
:
1 molar ratio was red-shifted to 585 nm, indicating the formation of larger Au-NPs. Compared with previous reports describing a SPR peak at 533 nm for ∼50 nm Au-NPs,29,30 the SPR peak of our Au-NP/MoS2 was red-shifted to 585 nm even though the particle sizes of the Au-NPs are close (∼50 nm). Such a shift would be due to the effective plasmon interactions of the Au–MoS2 composites31 and/or a partial covering and deformation of the spherical Au-NPs on the MoS2 surfaces as suggested by Polyakov et al.,32 in which the growth of Au-NPs on the surfaces of MoS2 might cause distortion of the spherical shape of the Au-NPs leading to a SPR peak red shift. Moreover, the disappearance of the typical absorption peak of the MoS2 in the composite with the molar ratio of 10
:
1 also derived from the aggregation of the Au-NP/MoS2 nanocomposites.
The thickness and surface morphologies of the Au-NP/MoS2 nanocomposites were examined using AFM. As shown in Fig. 3, the thickness of the pristine MoS2 nanoflakes was larger than 2 nm, indicating that the flakes have a multilayered structure since the thickness of typical single-layered MoS2 nanosheets is ∼0.7 nm.33 The AFM image of the Au-NP/MoS2 (1:
1 molar ratio) shows that the Au-NPs were aggregated at the edge of the large pieces of MoS2 nanoflakes, but did not cause large-scale aggregation of the MoS2, which is in agreement with the STEM results shown in Fig. 1C. Fig. 3C clearly proves that when the Au3+ ratio was increased to 10
:
1, many Au-NP/MoS2 aggregates were generated, and the thickness of the obtained composites was greater than 60 nm. The height profile of the AFM image indicates that the aggregated Au-NP/MoS2 nanocomposites have a porous structure. The Au-NP deposition on the MoS2 was also confirmed using EDX and XPS spectral measurements. The intensity of the Au peak in the EDX spectra (Fig. S2†) increased with the increase in the ratio of Au3+ to MoS2. In the XPS spectra (Fig. 4A), typical peaks of Mo 3d3/2 and 3d5/2 are observed at around 232.4 eV and 229.3 eV, respectively. There was no significant shift in the doublet peaks of the Mo 3d bands before and after the gold ion reduction, while we observed higher valence forms (Mo5+, Mo6+) using XPS (see ESI, Fig. S3 and Table S1†), suggesting partial oxidation of the MoS2 in the reduction process.34,35 The peaks in Fig. 4B located at ∼87.2 eV and ∼83.5 eV can be ascribed to Au 4f5/2 and Au 4f7/2, respectively, suggesting the reduction of the Au ions.10,14
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Fig. 3 AFM images of (A) the pristine commercial MoS2 nanoflakes, (B) Au-NP/MoS2 (with 1![]() ![]() ![]() ![]() |
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Fig. 4 XPS spectra of the (a) Mo 3d and (b) Au 4f regions of the pristine commercial MoS2 nanoflakes and the Au-NP/MoS2 with specified ratios. |
It is reported that MoS2 can adsorb AuCl4− to form a MoS2/AuCl4− redox pair, allowing spontaneous reduction of the Au3+ to Au-NPs (metal) and in situ growth on the MoS2 nanosheets.27 In addition, ethanol would be expected to enhance the reaction due to its reducing ability.29,36,37 To verify this possibility, a series of experiments was conducted changing the water/ethanol (v/v) ratios. For preparation of the samples, the MoS2 nanoflakes were collected by centrifugation to remove the solvent, then the precipitate was re-dispersed in water/ethanol solutions, which were sonicated for 1 h using a bath-type sonicator. A SEM image of the sample prepared in only water using the 5:
1 molar ratio of the Au ion precursor and MoS2 is shown in Fig. 5A, in which MoS2 nanoflakes were hardly observed, which implies that, in the absence of ethanol, the formed distorted MoS2 might cause compact aggregation of the Au-NPs. This idea is supported by the fact that the MoS2 works as a reducing agent. To further confirm this, XPS measurements were conducted and the obtained results (see ESI, Fig. S4†) demonstrated that when the Au-NPs were reduced by the MoS2, the Mo atoms were oxidized to higher valence forms (Mo5+ and Mo6+). When ethanol was involved in the reaction solution, the molar ratio of the Au ion precursor and MoS2 was fixed to 5
:
1 and the flake morphology of the MoS2 remained, as shown in Fig. 5B–E. As exhibited in the XPS results and the quantitative analysis, the amount of oxidized Mo decreased with the increase in the content of ethanol.
To elucidate the formation process of the Au-NP/MoS2 nanocomposites, time-dependent investigations of the morphological characterization were carried out. The samples for STEM observation were prepared at specified time intervals under similar reaction conditions. The series of STEM images (Fig. 6) shows the morphology at each reaction stage. After the first 5 min, a few small Au-NPs had formed on the edge of the MoS2. The number and size of the Au-NPs increased as the time progressed. On prolonging the reaction time to 20 min, the size of the Au-NPs was found to increase and flake-shaped nanocomposites began to assemble. Fig. 6D shows the morphology of the nanocomposites formed after 30 min, which reveals dense aggregation of the Au-NP/MoS2. As unbound sulfur is enriched at the edge of nanoflakes,38 the Au-NPs incorporated preferentially at the edge of the nanoflakes and large sized Au-NPs were produced. Because the larger Au-NPs have more active surfaces and a greater ability to bind sulfur,39 they would work as a joint to bind the sulfur to other pieces of MoS2 which would cause aggregation of the Au-NP/MoS2 nanocomposites. As shown in Fig. 6C, MoS2 nanoflakes with larger Au-NPs aggregated with each other, while the MoS2 nanoflakes with smaller Au-NPs did not exhibit such behaviour. Together with the obtained results, the formation process of the Au-NP/MoS2 nanocomposites can be proposed as schematically shown in Fig. 7.
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Fig. 6 STEM images the Au-NP/MoS2 samples (with 5![]() ![]() |
Due to the unique porous structure of our material, the Au-NP decorated MoS2 nanocomposites are expected to show a high surface-enhanced Raman scattering (SERS) performance. As shown in Fig. 8A, typical Raman peaks of R6G, for the bare Si substrate and prepared SERS substrates, appeared at ca. 1363 cm−1, 1509 cm−1 and 1650 cm−1 which were ascribed to the ν(C–C) stretching mode, and were in accord with reported R6G molecule SERS spectra.40 The intensity of the R6G signal was enhanced when using substrates with a higher content of Au-NPs. Significantly, there was an enhanced intensity for R6G on the Au-NP/MoS2 with the molar ratio of Au-NPs:
MoS2 = 10
:
1, and this sample exhibited the highest intensity. These results verify that the SERS effect strongly depends on both the increasing size of the Au-NPs and the aggregated nanoporous structure because morphology has an intimate link with so-called “hot spots”.41–44 To quantitatively study the SERS performance of the prepared nanocomposites, the analytical enhancement factor (EF) was calculated according to the following equation (eqn (1))25,45,46
EF = [ISERS]/[Ibulk] × [Nbulk]/[NSERS] | (1) |
The SERS intensities for different Au-NP/MoS2 nanocomposites were monitored for two different Raman peaks (1363 cm−1 and 1650 cm−1) of 10−5 M R6G to calculate the average enhancement factor of the prepared substrate, and the results are summarized in Table S3.† It was found that the Au-NP/MoS2 sample with a 10:
1 ratio exhibited the highest enhancement factor (19.9 × 105). Besides, R6G of different concentrations in the range of 10−4 to 10−7 M was applied to monitor the enhancement limit of the substrate which had the highest enhancement ability (Au-NP/MoS2 sample with 10
:
1 ratio). As shown in Fig. 8B, even at a concentration of R6G of 10−7 M, the peaks at 1363 cm−1 and 1503 cm−1 were still visible. As shown in Table S4,† the substrate had the highest enhancement factor of 73.4 × 105 when the concentration of R6G was 10−7 M.
To confirm the advantages of the 3D-nanocomposites, the SERS ability of pristine MoS2 nanoflakes, 2D-Au-NP/1T-MoS2 nanosheets and 3D-nanoporous Au-NP/MoS2 nanocomposites were compared and the results are shown in Fig. 8C. Although the charge transfer and dipole–dipole coupling of the semiconductor MoS2 sheets have been reported to enhance the Raman signal of molecules,47 the signal detected on the pristine MoS2 nanoflakes was extremely weak. In addition, in order to discuss the structural influence on the SERS, Au-NP/1T-MoS2 nanosheets with a 2D structure were also prepared as a control according to a previous report,27 in which, the Au-NPs were decorated on the surfaces of the MoS2 without aggregation, leading to the formation of 2D-structured Au-NP/MoS2 nanocomposites (denoted as 2D-Au-NP/MoS2). The Au-derived SPR peak of the 2D-Au-NP/MoS2 appeared at 580 nm, which is close to that of the 3D porous Au-NP/MoS2. As can be seen in the STEM, the average size of the Au-NPs in the 2D-Au-NP/MoS2 was ∼50.0 nm, which is similar to that (∼51.1 nm) of the Au-NPs of the 3D-Au-NP/MoS2. However, as shown in Table S3,† the EF of the 2D-Au NP/MoS2 was calculated to be 3.48 × 105, which is smaller than that (19.9 × 105) of the 3D porous Au-NP/MoS2 nanocomposites (19.9 × 105), even though the Au-NP sizes and the amount of Au-NP/MoS2 nanocomposites dropped on the Si substrate were the same, for which the deposited quantities were adjusted based on the absorbance in the UV/vis absorption spectra. It is suggested that the 3D porous architecture provided by the MoS2 frameworks would increase the specific surface area and increase the Z-distribution of the Au-NPs which would build up the amount of “hot spots” longitudinally as well as horizontally and enhance the SERS signal as observed in other studies.45,47
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra15421a |
This journal is © The Royal Society of Chemistry 2015 |