- Nano Express
- Open Access
Size Control and Growth Process Study of Au@Cu2O Particles
Nanoscale Research Lettersvolume 11, Article number: 390 (2016)
Au@Cu2O cuboctahedron with gold triangular nanoplate core and Cu2O shell was synthesized by a chemical method. X-ray diffraction (XRD) and transmission electron microscopy (TEM) tests demonstrated that the as-synthesis samples were consisted of gold triangular nanoplate core and Cu2O shell, and both of them were in good crystallization. The effective size control of the particles could be realized by controlling the amount of Au cores added in the synthetic process and Au@Cu2O particles with different shell thickness could be synthesized. The decrease of Cu2O shell thickness had a great difference in the optical performance, including blue shift of the resonant peaks and enhanced absorption intensity. The growth process from rough sheet structure to cuboctahedron was also explored. The results of photocatalytic degradation experiment showed that Au@Cu2O particles showed much better photocatalytic performance than that of pure Cu2O. The improved photocatalytic property of the Au@Cu2O particles was attributed to the comprehensive effect of the enhanced visible-light absorption and high separation rate of electron-hole pairs.
Photocatalyst can take advantage of solar power to generate redox couple for the degradation of organic pollutant. In recent years, many significant achievements about photocatalyst have been made [1–6]; however, photocatalyst still faces several problems which include low photocatalytic efficiency and unsuitable light absorption region. The former is mainly caused by the high recombination rate of electron-hole pairs, such as Bi2S3 , while the latter is attributed to the wide band gap, such as TiO2  and ZnO . The two disadvantages have seriously limited photocatalyst’s further applications. Thus, how to broaden the visible-light absorption range or promote electron-hole pairs separating has been an effective direction to push the research forward. The design of core-shell structure with suitable bandgap semiconductors seems to be a viable way to figure out these problems. In previous reports, Cu2O has been proved to be an ideal visible photocatalyst for its large light absorption coefficient, high refractive index and low cost [2, 10, 11]. However, the photocatalytic performance of pure Cu2O is far from satisfaction due to its wide size distribution and the high recombination rate of electron-hole pairs [12–14]. To get over these difficulties, modification of Cu2O with plasmonic nanoparticles seems to be an efficient way [2, 5, 15–21].
Plasmonic nanoparticles, especially noble metal, have strong localized surface plasmon resonance (LSPR) in the visible spectrum range, which arouses extensive interests into the preparation of high-efficiency plasmonic photocatalysts. Their LSPR can be further adjusted by controlling sizes, morphologies and surrounding dielectric environment. Compared with noble metal with other morphologies, triangular nanoplate (TN) has more efficient charge separation and red-shifted optical coefficient peak due to the integrated effect of its two-dimensional structure, sharp corners and anisotropy . These properties can improve the photocatalytic performance enormously. Thus, Au TN can be an excellent candidate for the modification of Cu2O. The heterogeneous nucleation of Cu2O not only helps overcome the shortcomings of large size and wide size distribution but also can tune its light absorption scope.
Reports about the construction of Au@Cu2O core-shell structure were abundant [5, 17–19], and various kinds of Au cores have been involved, such as sphere , rod , cube  and octahedron . However, as far as we know, few of them referred to the two-dimensional nanoplate core. Huang  and Mirkin  have prepared core-shell structure with triangular nanoplates as core. In their work, the core-shell heterostructures were successfully synthesized with good crystallinity. However, the morphology of the heterostructures only exhibited sheet structure, and the role of Au TN and the properties influenced by particle size have not been explored. Inspired by their work, we have designed a core-shell structure with triangular Au nanoplate core and Cu2O shell. Moreover, the shell thickness of the Au@Cu2O cuboctahedrons could be adjusted from 159 to 53 nm while symmetry and morphology of the cuboctahedrons were unaltered. Compared with the pure Cu2O, the photocatalytic property of the Au@Cu2O particles was improved greatly. The role of the Au TN, growth process, size control, optical properties and photocatalytic activity of the samples were analyzed in details.
Synthesis of gold TN
Gold TN was synthesized by the method reported with little modification . Briefly, 8 ml of 0.1 M hexadecyltrimethylammonium chloride (CTAC) was first added into a 100-ml conical flask with 40 ml of deionized water in it, and then 375 μl of 0.01 M KI was added. After the injection of 400 μl of 25.4 mM HAuCl4 and 100 μl of 0.1 M NaOH, the solution began to show light yellowish color. Then 400 μl of 64 mM ascorbic acid (AA) was added, and once AA was injected, the yellowish solution turned to colorless. At last, 50 μl of 0.1 M NaOH was added and stirred for several seconds. Then the reaction was left for 10 min without disturbance for complete crystalline growth. As the reaction proceeded, we could see the colorless solution turned to pink, then purple and at last blue. The triangular plates were detached and washed by centrifugation with deionized water. Then the Au TNs were attenuated into 3.1 ml.
Synthesis of Au@Cu2O Cuboctahedron
Au@Cu2O cuboctahedron was prepared by the method reported with little modification . In a 20-ml beaker, (8.9-x) ml of deionized H2O, 300 μl of 0.1 M CuCl2 solution, and 0.087 g of sodium dodecylsulfate (SDS) were added in sequence. Then x ml of the gold TN solution and 300 μl of 1 M NaOH solution were injected. Here, x stood for the volume of gold TN solution added. To get different shell thickness, the concrete values of x were set as 0, 0.1, 0.2, 0.4, 0.8, and 1.6, respectively. The total solution volume was kept at 10 ml. After stirring for 10 min, 500 μl of 0.2 M hydroxylamine hydrochloride (NH2OH·HCl) was added dropwise into the reaction solution. Two hours later after aging was finished, the product was gathered by centrifugation. The samples were designated as y-Au@Cu2O where y represented the shell thickness of the samples. Then the collection was washed with ethanol and deionized water several times to get rid of impurities ion and surfactant.
Characterization of the Samples
The crystalline phase of products prepared was identified by X-ray diffraction (XRD) with Cu-Ka radiation. Scanning electron microscopy (SEM) was taken on a S4800 SEM instrument. Transmission electron microscopy (TEM) and high-resolution transmission electron microscopy (HRTEM) (Hitachi H600A, Tokyo, Japan) were utilized to characterize structure. UV-3600 UV-vis-NIR spectrophotometer was used to characterize the UV-vis diffuse reflectance spectra. The specific surface areas of the samples were tested from nitrogen adsorption-desorption isotherms on a Micromeritics Tristar 3020 system.
The photocatalytic evaluation of the samples was carried out by dispersing 0.01 g of the product for the degradation of 100 ml MO solution (10 mg/l). A 500 W xenon lamp was chosen as visible-light source. Then the solution was stirred without light for 20 min to make sure that MO solution had got absorption equilibrium state. After every 20 min, 3–4 ml solution was taken out and centrifuged. UV-vis spectrophotometer was used to measure the product. The residual portion of MO could be worked out by the formula η = C/C 0 , where the original concentration and subsequent concentration of MO solution were respectively denoted as C 0 and C.
Reactive Species Trapping Experiments
Five millimolar triethanolamine (TEOA), isopropanol (IPA), and ascorbic acid (AA) were added to the MO solution as h+ scavenger, ·OH scavenger and ·O2 − scavenger, respectively. And the concentration of MO was measured after irradiation for 40 min. The degradation percentages of MO solution were calculated by the formula (C0 − C)/C0.
Results and Discussion
Phase and Crystal Structure Analysis
The XRD patterns of the samples were showed in Fig. 1a. The results distinctly demonstrated that there were two sets of diffraction data, which accorded well with the cubic Au (JCPDS no. 89-3697) and cubic phase Cu2O (JCPDS no. 05-0667). This indicated the synthesis of Au and Cu2O crystals. As shell thickness is decreasing, intensity of the Au peaks was getting stronger. Figure 1b was the SEM results of the samples, which displayed that the Au@Cu2O particles were uniformed cuboctahedrons with good monodispersity. TEM image (Fig. 1c) confirmed the formation of core-shell structure, and each cuboctahedron contained one Au TN. TEM image, size distribution histograms, and absorption spectrum of the pure Au TNs were showed in Additional file 1: Figure S1. The HRTEM image of the square regions illustrated the interplanar spacing of 2.13 and 2.48 Å, assigned to the spacing of the (2 0 0) and (1 1 1) plane of Cu2O. Moreover, the line scanning (Fig. 1e) of a single Au@Cu2O particle showed that gold element is principally located in the center of the particle while copper was bordered, which agreed well with the scanning transmission electron microscopy (STEM) (Fig. 1d) image.
Size Control and Growth Process Study
SEM images of the samples (Fig. 2a–f) showed that particles with six different sizes were synthesized by adding 0, 0.1, 0.2, 0.4, 0.8, and 1.6 ml of Au core solution, respectively. Accordingly, the average particle sizes of the samples were estimated to be 555 nm, 349 nm, 281 nm, 225 nm, 176 nm, and 137 nm, respectively.Considering the average particle size of the Au TN was 31 nm (Additional file 1: Figure S1b), the average shell thickness of the samples was 159, 125, 97, 72.5, and 53 nm, respectively. Therefore, accurate size control could be realized, due to the fact that each Au@Cu2O core-shell structure contained one Au core . As a result, a simple method was provided to adjust the thickness of Cu2O shell by altering the amount of the Au core in the synthetic process. The Au TN employed in the synthetic process was from the same batch, so the concentration of the seeds was invariable.
To explore the growth process of the samples, a series of experiments had been done. When 3.2 ml of Au solution was added, particles with rough sheet structure were synthesized (as shown in Fig. 3), instead of expected cuboctahedron smaller than 53-nm Au@Cu2O, because Au cores were too much to capture enough Cu2O particles for the growth of complete cuboctahedron shell. When 2.4 ml of Au TN was added, every Au core was provided with more Cu2O particles. And the intermediate structure was synthesized because more Cu2O particles could adsorb on the surfaces of Au TN core. When the volume of Au TN was decreased to 1.6 ml, complete cuboctahedron was synthesized. As the volume of Au TN sequentially decreased, the morphology of the Au@Cu2O core-shell structure was maintained as cuboctahedron with particle size increasing.
UV-vis and BET Analysis
Figure 4 represented the diffuse reflectance spectra of the samples. As the photograph showed (Additional file 1: Figure S2), the color of the reaction hydrosol was changing from dark orange to light green and then dark green. The distinct color change was obviously related to the core-shell interactions between Au TN core and Cu2O shell. Compared with the pure Cu2O, Au@Cu2O core-shell structure displayed strong absorption ability in the visible-light region. The absorption spectra at wavelength coverage below 500 nm were caused by the excitation interband transition of Cu2O shell. And the spectra at the wavelength coverage beyond 600 nm were attributed to the plasmon resonance of Au TN. In addition, with the shell thickness of Cu2O decreased, the plasmon peaks were blue-shifted drastically. The distinct blue-shift of the plasmon peak was because of the high refractive index and dielectric constant of the Cu2O shell. The plasmon resonance frequency of the noble metal was sensitive to the surrounding dielectric environment; therefore, the decrease of Cu2O shell thickness would cause blue-shift of the plasmon peak. Thus, Au@Cu2O core-shell heterostructure effectively adjusted the light absorption region of pure Cu2O and enhanced the visible-light absorption intensity.
Nitrogen adsorption-desorption isotherms from the Brunauer-Emmett-Teller (BET) test showed (Fig. 5) that the specific surface areas of pure Cu2O, 72.5-nm Au@Cu2O and 53-nm Au@Cu2O were 7.00, 13.10, and 17.72 m2/g, respectively. This result demonstrated that the Au@Cu2O particles had similar specific surface areas.
Photocatalytic Activity and Possible Mechanism
Figure 6a showed the degradation plots of MO involving photocatalytic activities of the samples. Compared with the pure Cu2O, Au@Cu2O particles showed better photocatalytic performance. As the shell thickness of the Au@Cu2O particles decreases, photocatalytic property was getting better. However, when the shell thickness was deceased from 72.5 to 53 nm, the photocatalytic property turned out to be worse. Thus, the 72.5-nm Au@Cu2O was found to exhibit the best catalytic performance, and after 80 min of the photoreaction, more than 86 % of MO was degraded.
The stability of the 72.5-nm Au@Cu2O was researched by degrading MO repeatedly, and the result was showed in Fig. 6b. The catalytic activity decreased slightly after each cycle, and considering the possible loss of catalysts during centrifugation, the stability was acceptable.
To investigate the roles that different active species played in the photocatalytic process, IPA, TEOA, and AA were chosen as scavengers of ·OH, h+, and ·O2 − in the trapping experiment. Figure 7a showed that after the addition of three scavengers, the degradation rates of MO were reduced from 80 to 75.1, 58, and 4.8 %, respectively. This result illustrated that ·OH and h+ were the main active species in the photocatalytic process, and ·O2 − had little effect on the photocatalytic activity.
Based on the above analyses, the electron generation and transfer processes of charge carriers in the Au@Cu2O particles were displayed in Fig. 7b. On one hand, the Schottky barrier formed at the metal and semiconductor interface functioned as electron sink to capture and shift photoexcited electrons from the Cu2O shell to the Au TN. The process was considered as direct electron transfer (DET) , which effectively reduced the recombination rate of electron-hole pairs and prolonged lifetime of the holes. On the other hand, the near-field electromagnetic coupling between the LSPR dipole of Au TN and the interband transition dipole of Cu2O caused plasmon-induced resonant energy transfer (PIRET) , which effectively promoted charge separation in the Cu2O shell. Therefore, the improved catalytic activity might be attributed to the synergetic effect of the DET and PIRET.
In summary, we have s Au@Cu2O core-shell structure with gold TN core and Cu2O shell. Moreover, the shell thickness of the core-shell particles could be controlled from 159 to 53 nm by adjusting the volume of Au solution. Photocatalytic experiment showed that Au@Cu2O core-shell structure exhibited better photocatalytic property than that of pure Cu2O, and the highest photocatalytic activity could be achieved on 72.5-nm Au@Cu2O which was 6.9 times better than that of pure Cu2O. The improved photocatalytic property was due to the integrated effect of the enhanced visible-light absorption and high separation rate of electron-hole pairs. This work would raise the possibility for exploring new core-shell structures and promote to probe more inspiring applications, apart from the field of photocatalysis, such as sensor or solar cell.
Liu J, Liu Y, Liu NY, Han YZ, Zhang X, Huang H, Lifshitz Y, Lee S, Zhong J, Kang ZH (2015) Metal-free efficient photocatalyst for stable visible water splitting via a two-electron pathway. Science 34:970–974
Meir N, Plante IJ, Flomin K, Chockler E, Moshofsky B, Diab M, Volokh M, Mokari T (2013) Studying the chemical, optical and catalytic properties of noble metal (Pt, Pd, Ag, Au)-Cu2O core-shell nanostructures grown via a general approach. J Mater Chem A 1:1763–1769
Ren ST, Wang BY, Zhang H, Ding P, Wang Q (2015) Sandwiched ZnO@Au@Cu2O nanorod films as efficient visible-light-driven plasmonic photocatalysts. ACS Appl Mater Interfaces 7:4066–4074
Chen XB, Liu L, Huang FQ (2015) Black titanium dioxide (TiO2) nanomaterials. Chem Soc Rev 44:1861–1885
Huang MH, Rej S, Chiu CY (2015) Facet-dependent optical properties revealed through investigation of polyhedral Au-Cu2O and bimetallic core-shell nanocrystals. Small 11:2716–2726
Li JT, Cushing SK, Bright J, Meng FK, Senty TR, Zheng P, Bristow AD, Wu NQ (2013) Ag@Cu2O core-shell nanoparticles as visible-light plasmonic photocatalysts. ACS Catal 3:47–51
Ge ZH, Zhang BP, Yu ZX, Jiang BB (2012) Controllable synthesis: Bi2S3 nanostructure powders and highly textured polycrystals. Cryst Eng Comm 14:2283–2288
Rai P, Majhi SM, Yub YT, Lee JH (2015) Noble metal@metal oxide semiconductor core@shell nano-architectures as a new platform for gas sensor applications. RSC Adv 5:76229–76248
Zhou XF, Lu J, Jiang JJ, Li XB, Lu MN, Yuan GT, Wang ZS, Zheng M, Seo HJ (2014) Simple fabrication of N-doped mesoporous TiO2 nanorods with the enhanced visible light photocatalytic activity. Nanoscale Res Lett 9:34
Sun SD (2015) Recent advances in hybrid Cu2O-based heterogeneous nanostructures. Nanoscale 7:10850–10882
Susman MD, Feldman Y, Vaskevich A, Rubinstein I (2014) Chemical deposition of Cu2O nanocrystals with precise morphology control. ACS Nano 8:162–174
Luo XL, Wang MJ, Yun L, Yang J, Chen YS (2016) Structure-dependent activities of Cu2O cubes in thermal decomposition of ammonium perchlorate. J Phys Chem Solides 90:1–6
Scuderi V, Amiard G, Boninelli S, Scalese S, Miritello M, Sberna PM, Impellizzeri G, Privitera V (2016) Photocatalytic activity of CuO and Cu2O nanowires. Mat Sci Semicon Proc 42:89–93
Zhang LM, Sun HQ, Xie L, Lu JN, Zhang LY, Wu SJ, Gao XS, Lu XB, Li JH, Liu JM (2015) Inorganic solar cells based on electrospun ZnO nanofibrous networks and electrodeposited Cu2O. Nanoscale Res Lett 10:465
Liu DY, Ding SY, Lin HX, Liu BJ, Ye ZZ, Fan FR, Ren B, Tian ZQ (2012) Distinctive enhanced and tunable plasmon resonant absorption from controllable Au@Cu2O nanoparticles: experimental and theoretical modelling. J Phys Chem C 116:4477–4483
Wiley BJ, Im SH, Li ZY, McLellan J, Siekkinen A, Xia YN (2006) Maneuvering the surface plasmon resonance of silver nanostructures through shape-controlled synthesis. J Phys Chem B 110:15666–15675
Yuan GT, Lu MN, Fei JH, Guo J, Wang ZS (2015) Morphologically controllable synthesis of core-shell structured Au@Cu2O with enhanced photocatalytic activity. RSC Adv 5:71559–71564
Yang YC, Wang HJ, Whang J, Huang JS, Lyu LM, Lin PH, Gwo S, Huang MH (2014) Facet-dependent optical properties of polyhedral Au-Cu2O core-shell nanocrystals. Nanoscale 6:4316–4324
Wang WC, Lyu LM, Huang MH (2011) Investigation of the effects of polyhedral gold nanocrystal morphology and facets on the formation of Au@Cu2O core@shell heterostructures. Chem Mater 23:2677–2684
Wang HJ, Yang KH, Hsu SC, Huang MH (2016) Photothermal effects from Au-Cu2O core-shell nanocubes, octahedra, and nanobars with broad near-infrared absorption tenability. Nanoscale 8:965–972
Lu B, Liu AP, Wu HP, Shen QP, Zhao TY, Wang JS (2016) Hollow Au-Cu2O core-shell nanoparticles with geometry-dependent optical properties as efficient plasmonic photocatalysts under visible light. Langmuir 32:3085–3094
Kuo CH, Hua TE, Huang MH (2009) Au nanocrystal-directed growth of Au-Cu2O core-shell heterostructures with precise morphological control. J Am Chem Soc 131:17871–17878
Xue C, Chen XD, Hurst SJ, Mirkin CA (2007) Self-assembled monolayer mediated silica coating of silver triangular nanoprisms. Adv Mater 19:4071–4074
Chen L, Ji F, Xu Y, He L, Mi YF, Bao F, Sun BQ, Zhang XH, Zhang Q (2014) High-yield seedless synthesis of triangular gold nanoplates through oxidative etching. Nano Lett 14:7201–7206
Kong L, Chen W, Ma DK, Yang Y, Liu SS, Huang SM (2012) Size control of Au@Cu2O octahedra for excellent photocatalytic performance. J Mater Chem 22:719–724
Furube A, Du LC, Hara K, Katoh R, Tachiya M (2007) Ultrafast plasmon-induced electron transfer from gold nanodots into TiO2 nanoparticles. J Am Chem Soc 129:14852–14853
Cushing SK, Li JT, Meng FK, Senty TR, Suri S, Zhi MJ, Li M, Bristow AD, Wu NQ (2012) Photocatalytic activity enhanced by plasmonic resonant energy transfer from metal to semiconductor. J Am Chem Soc 134:15033–15041
This work was supported by the Synthesis of high-emissivity far infrared nanocomposites and its application in the functional modification of silk fibers (P110900213) and Testing and Analysis Center Soochow University.
The experiments were guided by YW in this work, and all the processes were designed by ZW and MZ. SL participated in the discussion and gave useful suggestions. The manuscript was composed by YW. All authors read and approved the final manuscript.
The authors declare that they have no competing interests.
(a) TEM image. (b) Particle size histograms and UV-is spectra of the Au triangular nanoplate (TN) colloids. Figure S2. Photograph of colloidal suspensions of the samples. (DOCX 443 kb)