World Journal Of Engineering Cr nanostructures fabricated based on porous anodic alumina membranes Hany Hamdy 1*, Sang-Wan Ryu 2, Mohamed Shaban 1† 1 Department of Physics, Faculty of Science, Beni-Suef University, Beni-Suef, Egypt 2 Department of Physics, Chonnam National University, Gwangju, South Korea * E-mail: † hshamdy@hotmail.com, E-mail: mssfadel@yahoo.com; mshaban_bsu@bsu.edu.eg In this paper, we propose an efficient and effective method to fabricate highly ordered Cr nanoarrays of different morphologies. Nanoporous hexagonal array of Cr nanoparticles with sub-gaps less than 15 nm and particle size less than 50 nm are fabricated on the top surface of porous anodic alumina membrane (PAA) fabricated with the assistance of cathodic polarization and pore widening process. In addition, V-Shape Cr-nanoarrays are fabricated on the top surface of PAA membrane prepared without the assistance of cathodic polarization and pore widening. A field emission scanning electron microscope (FE-SEM) and atomic force microscope (AFM) were used to characterize the morphologies and structures of the Cr nanoarrays and the PAA membranes. 1. INTRODUCTION In recent years, fabrication of noble metal nanoarrays has attracted much interest owing to their potential use in many applications.1,2 However, there is a strong demand for cheap and reliable material that can be patterned in two and three dimensions. We believe that chromium is in many ways an excellent material for fabrication of nanostructures. The grain size is typically very small (of order 5 nm or less), the surface mobility is very low, and the stability under exposure to air is excellent. In addition, Chromium has found various applications in many fields including metallurgy, catalysis, magnetic fields, and semiconductors.3-6 Moreover, it is widely accepted that 2D and 3D nanostructures are important components for nanoscale devices with many promising applications, due to their large surface areas and other unique properties.7-9 In other hand, porous anodic alumina (PAA) membranes have been widely used as templates in the fabrication of various nanostructures because of the cheap equipment, easy technology, high-throughput, and high controllability of the process.10,11 Consequently, it will be very interesting to fabricate 2D Cr nanoarrays based on PAA membranes. 2. EXPERIMENTAL DETAILS Two step anodization was utilized to fabricate highly ordered PAA membranes. 10,11 The first anodization process was performed at 40 V in 0.3 M oxalic acid at 9 oC for 3 h. After the removal of the aluminum oxide, the second anodization was performed at the same conditions for 5 min followed by barrier-thinning process.11 In order to study the effects of the combined cathodic polarization and pore widening processes on the morphology of the fabricated Cr nanostructures another set of samples was fabricated with the assistance of 10 min cathodic polarization and 70 min pore widening process under the same experimental conditions.11 393 Cr thin layers were sputtered on the PAA membranes by means of r.f. magnetron sputtering. Magnetron sputtering was carried out in pure argon with an r.f. power of 150 W for varying amounts of time. The total gas pressure during deposition was 5 mTorr. The substrate temperature during the sputtering was set at room temperature. A field emission scanning electron microscope (FESEM), and atomic force microscopy (AFM) were used to characterize the morphologies and structures of the PAA membranes and the sputtered thin films. 3. RESULTS AND DISCUSSION 3.1. Nanoporous hexagonal array of Cr nanoparticles Figure 1(a) illustrates a typical SEM top view of PAA membrane anodized for 5 min and pores widened for 70 min after 10 min cathodic polarization. Hexagonal aligned nanopores were formed in the PAA membrane. The pore diameter is about 79 nm, the interpore distance is 100 nm, and the pore density is approximately 1.1 × 1010 cm-2. A scraggly surface with nanoprotuberances can be seen clearly at the oblique view AFM of the PAA membrane as shown in figure 1(b). Around each nanopore there are six active nanodots with a hexagonal arrangement.12 Fig. 1. (a) Top view SEM image and (b) oblique view AFM image of blank PAA membrane anodized for 5 min and pores widened for 70 min after 10 min cathodic polarization. World Journal Of Engineering Figs. 2(a) and (b) show oblique view AFM images of PAA membranes anodized for 5 min and sputter-coated with Cr for 40 and 120s, respectively. The insets of Figs. 2(a) and ( b) show top view SEM images. It is seen that each of the six active dots surrounding the pores have acted as seed for growing a Cr nanoparticle on top of PAA membrane. There are also very narrow gaps, sub-gaps ≤ 15 nm, between the neighboring Cr nanoparticles as seen in the oblique and cross-sectional SEM images in Fig.2(c and d). The possibility of tuning the size of these nanoparticles as well as the distance between them is depending on the length of the sputtering time. Additionally, the pore center surrounded, and to some degree covered, by the Cr nanoparticles. The mean height of the Cr nanoparticles is increased from 30 to 70 nm whereas the diameter is increased from 35 to 49 nm with increasing the sputtering time from 40 to 160sec. The mechanism of formation of nanoparticles by self agglomeration on porous anodic alumina membranes was discussed in our previous report.13 23 nm. This can be attributed to the conformable and tight adherence of the Cr film to the pore surface. In addition, the rate of growth of V-shape height is estimated to be ~ 0.113nm/s. Fig.3. SEM images of PAA template anodized for 5 min (a) top view, and (b) cross-sectional view. Fig.4. Cross-sectional SEM images of PAA membranes, anodized for 5 min after sputtering with Cr for (a) 80, and (b) 160 sec. 4. CONCLUSION Aligned 2D- Cr nanostructures have been fabricated on surface of PAA membranes by r.f. magnetron sputtering. The sputtering time and PAA structural parameters can have great effects on the morphology of the resulting nanostructures. The synthesis method used in this study has several merits such as low cost, mass production, reduced impurities, and tailored dimensions of the resulting Cr nanostructures. Fig.2. AFM images of PAA membranes after sputter-coating with Cr for (a) 40, (b) 120 sec; (c) oblique angle and (d) cross- sectional view SEM. The insets of (a and b) show top view SEM images. 3.2 V-Shape Cr nanoarrays Figure 3 illustrates SEM images (a) top view and (b) cross-sectional view of blank PAA membrane anodized for 5 min and prepared without the assistance of cathodic polarization and pore widening processes. The pore diameter is about 31 nm, whereas the interpore distance and the pore density are the same as in Fig.1. In this case the six active dots around each nanopore are grown with larger size but not sharper as in Fig.1. Figure 4 shows cross-sectional SEM images of PAA membranes sputter-coated with Cr for 80, and 160s, respectively. It is seen that each of the six active dots surrounding the pores have acted as seed for growing a Cr nanoparticle on top. In this case, the size of the active dots is very large and distance between them is very small, so the neighbored Cr nanoparticles are side-by-side coalescence and tailored to the "V" shape as the sputtering time increases. From the microscopic analysis of the SEM images, a reduction in the pore diameter is observed from about 31 to References 1. Y. B. Zheng, and T. J. Huang, Journal of the Association for Laboratory Automation 13, 215 (2008). 2. M. Pelton , J. Aizpurua , and G. Bryant, Laser & Photonics Reviews 2, 136(2008). 3. M. J. Udy, Chromium: Metallurgy of Chromium and Its Alloys, vol. II: Reinhold, NewYork, 1956) 4. G. W. Mbise, D. L. Bellac, G. A. Niklasson, C. G. Granqvist, J. Phys. D, Appl. Phys. 30, 2103 (1997) 5. R. D. Tilley, D. A. Jefferson, J. Mater.Chem. 12, 3809 (2002) 6. W. S. Zhang, E. Bruck, Z. D. Zhang, O. Tegus, W. F. Li, P. Z. Si, D. Y. Geng, K. H. J. Buschow, Physica B 358, 332 (2005) 7. Z. L. Wang, Z. W. Pan, Adv. Mater. 14(15), 1029 (2002) 8. L.S. Zhong, J.S. Hu, H.P. Liang, A.M. Cao, W.G. Song, L.J. Wan, Adv. Mater. 18, 2426 (2006) 9. K. Zhang, C. Rossi, C. Tenailleau, P. Alphonse, Appl. Phys. Lett. 92(6), 063123 (2008) 10. M. Shaban, H. Hamdy, F. Shahin, and S.-W. Ryu, J. 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