22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Plasma-vapour-deposition synthesis of Au, Ag and AuAg core-shell nanoparticle on metal oxide semiconductors S. Peglow1, M.-M. Pohl2, A. Kruth1 and V. Brüser1 1 Leibniz-Institute for Plasma Science and Technology e.V., Felix-Hausdorff-Strasse 2, DE-17489 Greifswald, Germany 2 Leibniz-Institute for Catalysis e.V., Albert-Einstein-Strasse 29a, DE-18059 Rostock, Germany Abstract: Due to their exceptional optical properties noble metal nanoparticles are of interest for various applications. A novel synthesis method for the production of homogenous nanoparticles using a combination of plasma vapour deposition and a subsequent thermal annealing process is presented. The optical and morphological properties of gold, silver and gold-silver core-shell particles on titania semiconductor are investigated. Keywords: core-shell nanoparticles, plasma-vapour deposition, solid state dewetting 1. Introduction Noble metal nanoparticles are used in a variety of fields such as photocatalytic applications [1], surface plasmon resonance spectroscopy [2], information technology [3], environmental protection [4], biochemical sensing [5] and cancer treatment [6]. Commonly, gold nanoparticles are produced via chemical methods (Turkevich [7], Brust [8]). Similar proceedings are taken for silver nanoparticle synthesis [9]. Core-shell particles consist of a core and a differently composed outer shell. The material combination sequence and elemental ratio determine the properties of these hybrid structures and their applications in catalysis [10], photoluminescence [11,12], biomedicine (drug delivery [13] and controlled release [14], bioimaging [11]), pharmacy [15] and photonic crystals [16]. Because of its biocompatibility, preferred optical properties and protection of the core material from corrosion and oxidation, gold is favoured as shell material. Choosing silver as an outer layer results in antibacterial properties [17]. Combining two metals that are known for their plasmonic activity and tuning their elemental ratios enables to shift the resulting plasmon resonance frequency between the resonance frequencies of both materials involved [6]. This work presents a novel and easy synthesis method for monometallic and bimetallic core-shell nanoparticle production using conventional magnetron sputtering and subsequent thermal annealing. This method combination takes advantage of a process referred to as solid state dewetting describing nanoparticle formation through annealing of thin metal films [18]. Radio frequency (RF) magnetron sputtering produces homogeneous layers [19] ensuring high control over nominal metal layer thickness preparation and thus a direct influence on nanoparticle size after annealing [20]. Since research in metalsemiconductor photocatalysis using Au, Ag and AuAg core-shell particles emerged in recent years, the investigated particles were deposited on titanium dioxide semiconductor substrates. O-1-1 2. Experimental As a substrate a 270 nm thick TiO 2 layer was deposited by a reactive direct current (DC) magnetron sputtering process onto rough fluorine doped tin oxide (FTO, TCO 22-7, Solaronix) on soda lime glass. For the deposition of gold and silver metals, two 2 inch sputtering targets (both 99,999%, MaTeck) were used. To create nanoparticles, the metal/TiO 2 samples were put straight into a quartz tube furnace for thermal annealing (no temperature ramp was applied; all samples were annealed for 30 min in an oxygen atmosphere). For pure Au and AuAg/TiO 2 samples 400°C was applied, whereas the silver layer was treated at 200°C. To decrease their size distribution the gold nanoparticles synthesis was divided into two repeated deposition/annealing steps leading to particles of 10-30 nm in diameter. For AuAg core-shell structures, a gold layer was deposited on top of a silver layer before the whole sample was thermally treated. The AuAu ratio was varied by tuning the initial layer thickness of gold and silver films. For transmission electron microscopy (TEM) measurements, a 30 nm thick TiO 2 layer was sputter-deposited onto silicon nitride grids applying the same PVD method as described above. 3. Results and Discussion Due to the rough morphology of the titania substrate, the deposited gold film did not form a fully continuous layer. After application of the annealing treatment, the semi-continuous gold film reshaped into discrete Au nanoparticles, see scanning electron microscopy (SEM) image in Fig. 1. Their particle size seemed to depend on their three dimensional location on the titania surface. Large particles formed on top of the TiO 2 columns whereas smaller particles are located in the intercolumnar space. 1 nanoparticles at 520 nm is originated in the interaction with the titania environment. Additionally, a shift of the absorption band to higher wavelength can be observed at repetitions of the deposition-annealing steps. Due to the optical cut-off of the substrate, the LSPR of silver nanoparticles could not be observed in this system. Regarding core-shell nanoparticles and considering the limitations of the before mentioned optical cut-off at the silver LSPR frequency, an increase in silver amount led to a decreases in absorption at higher wavelength. This proved that a change in the elemental ratio of gold silver core-shell nanoparticles effected their optical properties. Fig. 1. SEM image of Au nanoparticles on titan dioxide after two cycles of subsequent RF-magnetron sputtering and thermal annealing. In contrast, the deposition of silver at similar loadings as for gold immediately resulted in the formation of separate islands. Thermal annealing at 200°C led to a reduction in the nanoparticle size from 10-40nm to 510nm, as well as a decrease in size distribution and concentration of Ag nanoparticles on top of the titania nanocolumns. The last phenomenon can be explained with Ag diffusion commencing at 200°C and occurring more pronounced at 400°C. AuAg core-shell nanoparticles were prepared and compared for three different elemental ratios (3:1; 1:1 and 1:3, respectively).The observed particles can be roughly divided into larger particles with a main diameter of 1020 nm and multiple small nanoparticles around and below 3 nm (both derived from SEM images not shown here) in size. An increase of the gold amount in the coreshell nanoparticles led to an increase in number of large particles. TEM images confirmed the increase in size for large particles from Ag/Au (1:1) to Ag/Au(1:3). However, at the lowest Au amount, Ag/Au (3:1), large irregularly shaped particles are observed. The number of small particles seems to increase with increasing silver content. Energy dispersive x-ray spectroscopy (EDX) measurements confirmed that the large particles consist of a gold core surrounded by a silver shell. The small nanoparticles appeared to be almost entirely silver containing. A higher silver ratio at the preparation resulted in an increase in silver shell thickness and in a decrease in the gold core diameter. Additionally, multicore nanoparticles consisting of several small gold cores encapsulated in one silver shell were observed. The absorption properties of the gold, silver and goldsilver core-shell particles can be explained by localized plasmon resonance. A broadening of the absorption peak at 620 nm for gold nanoparticles was observed due to a significant particle size distribution. The red-shift of the absorption peak compared to the localized surface plasmon resonance (LSPR) frequency of isolated Au 2 4. Conclusion A synthesis method for the preparation of monometallic and bimetallic core-shell nanoparticles combining a conventional magnetron sputtering process with a thermal annealing procedure was presented. Tuning of the process parameter allows for adjusting the optical and structural properties of the nanoparticles. Due to alternative sputtering of silver and gold the formation of core-shell nanoparticles with adjustable shell thickness could be realized. 5. Acknowledgement This work was funded by the German Research Foundation (DFG). We would like to thank Daniel Köpp for PVD of the TiO 2 substrate, Anja Albrecht for XRD measurements, and Dr. Harm Wulff from University of Greifswald for the crystallite size calculation. 6. References [1] X. Zhang, Y. L. Chen, R.-S. Liu and D. P. Tsai. Rep. Prog. Phys., 76 (2013) [2] K. A. Willets and R. P. Van Duyne. Annu. Rev. Phys. Chem., 58(2007) [3] E. Ozbay. Science, 311 (2006) [4] G. A. Mansoori, T. R. Bastami, A. Ahmadpour and Z. Eshaghi. Annual Review of Nano Research, 2 (2008) [5] A. El-Ansary and L. M. Faddah. Nanotechnol., Sci. Appl., 3 (2010) [6] J. Conde, G. Doria and P. Baptista. J. Drug Delivery, 2012 (2012) [7] J. Kimling, M. Maier, B. Okenve, H. Kotaidis, H. Ballot and A. Plech. J. Phys. Chem. B, 110 (2006) [8] M. Brust, J. Fink, D. Bethell, D. J. Schiffrin and C. Kiely. J. Chem. Soc., Chem. Commun. (1995) [9] M. G. Guzmán, J. Dille and S. Godet. Int. J. Chem. Bio. Eng., 2, 3 (2009) [10] Q. Zhang, I. Lee, J. B. Joo, F. Zaera and Y. Yin. Acc. Chem. Res., 46 (2012) [11] E. von Haartman, H. Jiang, A. A. Khomich, J. Zhang, S. A. Burikov, T. A. Dolenko, J. Ruokolainen, H. Gu, O. A. Shenderova, I. I. Vlasov et al. J. Mater. Chem. B, 1 (2013) [12] C. L. Yuan and P. S. Lee. EPL, 83 (2008) O-1-1 [13] N. K. Verma, K. Crosbie-Staunton, A. Satti, S. Gallagher, K. B. Ryan, T. Doody, C. McAtamney, R. MacLoughlin, P. Galvin, C. S. Burke et al. J. Nanobiotechnol., 26 (2013) [14] J. Yang, D. Shen, L. Zhou, W. Li, X. Li, C. Yao, R. Wang, A. M. El-Toni, F. Zhang and D. Zhao. Chem. Mater., 25 (2013) [15] D. Wang, J. He, N. Rosenzweig and Z. Rosenzweig. Nano Lett., 4 (2004) [16] K. P. Velikov, A. Moroz and A. van Blaaderen. Appl. Phys. Lett., 80 (2002) [17] M. Banerjee, S. Sharma, A. Chattopadhyay and S. S. Ghosh. Nanoscale, 3 (2011) [18] C. M. Mueller and R. Spolenak. Acta Mater., 58 (2010) [19] S.-H. Jeong, B.-S. Kim, B.-T. Lee, H. R. Park and J.K. Kim. J. Kor. Phys. Soc., 41 (2002) [20] T.-W. Chang, M. R. Gartia, S. Seo, A. Hsiao and G. L. Liu. Nanotechnology, 25 (2014) O-1-1 3
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