Structural and optical characterization of spinel type cobalt oxide nanoparticles embedded in amorphous silicon oxide matrix prepared by a hybrid PVD /PECVD process Karthika Lakshmi Kolipaka1, Volker Brueser1, Antje Quade1, Jan Schaefer1, Harm Wulff2, Franz Faupel3 1 Leibniz Institute for Plasma Science and Technology, INP Greifswald e.V., Felix-Hausdorff-Str. 2, 17489 Greifswald, Germany; 2Ernst Moritz Arndt University Greifswald, Institute of Physics, Felix-Hausdorff-Str. 6, 17489 Greifswald, Germany; 3University of Kiel, Institute for Materials Science – Multicomponent Materials, Kaiserstr.2, 24143 Kiel, Germany Abstract: Composite materials consisting of semiconducting nanoparticles embedded in a dielectric matrix have attracted a great deal of attention because of their use in catalytic, gas-sensing, optical and magnetic applications. In this work, a combination of physical vapour deposition (PVD) and plasma enhanced chemical vapour deposition (PECVD) techniques is employed. Preparation of nanosized spinel type cobalt oxide particles embedded in an amorphous silicon oxide matrix (Co3O4-SiOx composite) has been carried out by RF magnetron sputtering of cobalt and simultaneous plasma polymerization of hexamethyldisilazane (HMDSN) and further calcination. Phase composition studied using X-ray diffraction (XRD) analysis reveals the presence of crystalline Co3O4 with an average particle size of around 35-45 nm. The bonding nature of the film investigated using X-ray photoelectron spectroscopy (XPS) and Fourier transform infrared spectroscopy (FTIR) reveals silicon oxide as the dominant chemical composition of the matrix. The SEM micrograph depicts the amorphous and porous nature of the composite surface. The optical properties are similar to that of spinel type cobalt oxide with absorption peaks around 475 nm and 775 nm. The Tauc’s plot indicates the energy band gap for direct allowed transition as 1.95 eV and 1.38 eV. These obtained values are close to previously reported values. Keywords: PVD/PECVD, nanocomposites, spinel type cobalt oxide, hexamethyldisilazane, silicon oxide 1. Introduction The use of spinel type cobalt oxide is found in many applications such as catalysts, supercapacitors, phosphate ion sensors and CO sensors [1-4]. Especially cobalt oxide dispersed in amorphous silica matrix provides interesting applications such as optical sensors [5]. In the following contribution we present the preparation of nano sized spinel type cobalt oxide embedded in an amorphous silicon oxide matrix. 2. Experimental Initially Co – a: SiCNH nanocomposites have been prepared by the sputtering of cobalt (PVD) and simultaneous plasma polymerization of hexamethyldisilazane (HMDSN) (PECVD) (submitted elsewhere). The process was carried out in an RF magnetron sputtering system operating at 13.56 MHz frequency. These Co – a: SiCNH nanocomposites are calcinated in ambient air at 500°C for 2h. The calcination yielded in the formation of nanosized spinel type cobalt oxide particles embedded in amorphous silicon oxide matrix. Phase composition of the composites prepared on borosilicate glass was investigated using Xray diffraction (XRD) using CuKα radiation (θ2θ Diffractometer Siemens D5000). The measurements were made in grazing incidence set at an angle of 0.5° to the sample surface. The chemical bonding on the composite surface was studied using X-ray photoelectron spectroscopy (XPS). X-ray photoelectron spectrophotometer Axis Ultra, Kratos, Manchester, GB was used to analyze composites prepared on borosilicate glass. A monochromatic X-ray radiation of Al Kα was used. For the wide scan measurement 150 W X-ray radiation was used with pass energy of 80 eV. For the high resolution measurement 225W X-ray radiation with pass energy of 10 eV was used. Charge neutralization was applied. All the spectra were referenced to the aliphatic carbon at binding energy of 285.0 eV. The topography of composites prepared on aluminum substrate was studied using scanning electron microscopy (SEM) with a backscattered electron detector. Fourier transform infrared spectra (FTIR) of the composites prepared on aluminum substrate were taken using Perkin Elmer spectrometer in attenuated total reflection (ATR) mode. Optical absorption measurements of the composites were performed using a UV-Vis spectrophotometer (Analytik Jena) in 1 cm cuvettes. For this the composites were prepared on borosilicate glass. The XRD pattern shows sharp peaks which correspond to Co3O4. It represents crystalline Co3O4 with only small broadened profiles of all measured reflections. Only small broadened profiles correspond with nearly perfect crystals (that means only small lattice defects) as well as large particle sizes. From the pure physical line profile (Fourier transforms) the mean particle sizes was calculated to be of 35 nm, from the Williamson-Hall plot mean particle sizes of 45 nm was obtained. No peaks corresponding to SiOx are found in the XRD pattern. The FTIR results discussed further indicate the presence of SiOx bonds. XRD and FTIR results together indicate that silicon oxide is not present in crystalline form. XPS Fig 2 gives the survey scan XPS spectrum of the Co3O4-SiOx composite. The elements cobalt, oxygen, silicon, and carbon are detected on the surface of the composite. 3. Results and discussion XRD X-ray diffraction pattern obtained for the Co3O4-SiOx composite is shown in Fig 1. Figure 2. Survey scan XPS spectrum of Co3O4-SiOx composite. Figure 1. XRD pattern of Co3O4-SiOx composite. The highly resolved measured spectra of C 1s, Si 2p, and Co 2p3/2 peaks are studied further. Fig 3 depicts the highly resolved measured spectrum of the Si 2p peak. The binding energy of the Si 2p peak represents Si(-O)2 and Si(-O)3 bindings[6]. The chemical composition of the matrix is dominated by SiOx bonds [6, 7] which is further supported by the FTIR results discussed below. The highly resolved measured spectrum of Co 2p3/2 peak shows presence of cobalt oxides on the surface of the composite. the presence of amorphous silicon oxide is confirmed with the FTIR spectrum (as no silicon oxide bonds were observed in the XRD results, indicating that no crystalline silicon oxide is present). Therefore it can be said that nano sized spinel type cobalt oxide particles are embedded in the amorphous silicon oxide matrix. This presents an interesting incorporation of magnetic particles inside an amorphous matrix. SEM The SEM micrograph of the Co3O4-SiOx composite is depicted in Fig 5. Figure 3. Highly resolved measured Si 2p peak of Co3O4-SiOx composite. ATR-FTIR The ATR-FTIR spectrum of the composite shows several characteristic bonds corresponding to silicon oxide. Fig 4 shows the ATR-FTIR spectrum of the Co3O4-SiOx composite. Figure 5. SEM micrograph of Co3O4-SiOx composite. Scale is show in the picture. The SEM micrograph in Fig 5 indicates the porous and amorphous nature of the surface of Co3O4-SiOx composite. The crystalline Co3O4 nanoparticles can be observed as crystals in some areas of the micrographs. Optical measurements Figure 4. ATR-FTIR spectrum of Co3O4-SiOx composite. Several peaks in the FTIR spectrum correspond to silicon oxide bonds. The peaks at 1100 cm-1 and 960 cm-1 correspond to SiO asymmetric stretching vibrations. The peak at 680 cm-1 corresponds to Si-H bending vibrations. Thus The optical absorption spectrum of Co3O4 and Co3O4-SiOx composite is shown in Fig 6. The absorption spectrum of Co3O4 is included for comparison. In the absorption spectrum of Co3O4 peaks are observed around 475 and 775 nm. The same peaks are also observed in the Co3O4-SiOx composites, but, the peak at 475 nm is not as significant as in the pure Co3O4. This can be because of the influence of the silicon oxide matrix. But, however, the absorption spectrum is similar to that of pure Co3O4. 4. Conclusion Spinel type Co3O4 nanoparticles of average size 35-45 nm embedded in amorphous silicon oxide matrix have been prepared using a hybrid PVD/PECVD process and further calcination. The structural, topological, and optical properties of the Co3O4-SiOx composites were studied. References [1] W. Jia et al., J. Electroanal. Chem. 625, 27 (2009). [2] V. R. Shinde et al., Appl. Surf. Sci. 252, 7487 (2006). [3] Y. Shimizu, Y. Furuta, Solid State Ionics 113115, 241 (1998). Figure 6. Optical absorption spectra of Co3O4 and Co3O4-SiOx composites. The Tauc plot of (αhν) 2 vs hν is shown in Fig 7. Upon extrapolation of the curve it intercepts the X-axis at 1.38 eV and 1.95 eV. This gives the energy band gap for direct allowed transition as 1.95 eV [8]. Similar results are reported elsewhere [9]. Thus the crystalline Co3O4 nanoparticles embedded in the amorphous silicon oxide matrix are characterized with direct band gap energies of 1.95 eV and 1.38 eV. Figure 7. Plot of (αhν) 2 vs hν of Co3O4-SiOx composites. [4] M. Ando et al., J. Mater. Chem. 7, 1179 (1997) [5] L. Armelao et al., J. Non-Cryst. Solids 293-295, 477 (2001). [6] D. S. Wavhal et al., Plasma Processes Polym. 3, 276 (2006). [7] E. Vasallo et al., Appl. Surf. Sci. 252, 7993 (2006). [8] R. Drasovean et al., J. Non-Cryst. Solids 352 (920), 1479 (2006). [9] F Gu, C Ki, Y Hu, L Zhang, J. Cryst. Growth 304, 369 (2007).
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