Proceeding of ICNM - 2009properties of a photonic crystal [2]. Moreover porous silicon possesses the...

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10 *************************************************************************** Porous silicon – nanomaterial with embedded magnetic nanostructures Petra. Granitzer (1) , K. Rumpf (1) , P. Poelt (2) , M. Albu (2) (1) Institute of Physics, Karl Franzens University Graz, Universitaetsplatz 5, 8010 Graz, Austria (2) Institute for Electron Microscopy, University of Technology Graz, Steyrergasse 17, 8010 Graz, Austria Abstract : A semiconductor/metal nanocomposite is composed of a porosified silicon wafer and embedded ferromagnetic nanostructures. Porous silicon (PS) achieved by anodization of a highly doped silicon wafer offers oriented pores grown perpendicular to the surface and clearly separated from each other. Within the pores of the porous silicon matrix ferromagnetic nanostructures are precipitated. The obtained hybrid system merges the electronic properties of silicon with the magnetic properties of the incorporated ferromagnetic metal. On the one hand such a magnetic system can be achieved by electrochemical deposition of a transition metal from a metal salt solution into the pores of the nanostructured silicon skeleton. On the other hand magnetic particles of a few nanometers in size, fabricated in solution, can be incorporated by immersion. The electrochemically deposited nanostructures can be tuned in size, shape and their spatial distribution by the process parameters and thus specimens with desired ferromagnetic properties can be fabricated. Using magnetite nanoparticles for infiltration into porous silicon is not only of interest because of the magnetic properties of the composite material due to the possible modification of the ferromagnetic/superparamagnetic transition but also because of the biocompatibility of the system caused by the low toxicity of both materials. Thus it is a promising candidate for biomedical applications as drug delivery or biomedical targeting. Introduction : Nanostructuring of materials results in a drastic change of their intrinsic properties. For example porous silicon achieved by anodization of a silicon wafer offers physical properties which can not be observed in case of bulk silicon. Microporous silicon which exhibits interconnected channels with diameters between 2 nm and 4 nm shows a strong luminescence in the visible [1] caused by quantum confinement effects. Macroporous silicon offers properties of a photonic crystal [2]. Moreover porous silicon possesses the ability to biodegrade within body fluids [3] and is known as a bioactive material [4], two properties Proceeding of ICNM - 2009 1 st International Conference on Nanostructured Materials and Nanocomposites (6 – 8 April 2009, Kottayam, India) Published by : Applied Science Innovations Private Limited, India. http://www.applied-science-innovations.com

Transcript of Proceeding of ICNM - 2009properties of a photonic crystal [2]. Moreover porous silicon possesses the...

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Porous silicon – nanomaterial with embedded magnetic nanostructures

Petra. Granitzer (1), K. Rumpf (1), P. Poelt (2), M. Albu (2)

(1) Institute of Physics, Karl Franzens University Graz, Universitaetsplatz 5, 8010 Graz, Austria

(2) Institute for Electron Microscopy, University of Technology Graz, Steyrergasse 17, 8010 Graz, Austria

Abstract : A semiconductor/metal nanocomposite is composed of a porosified silicon wafer and embedded ferromagnetic nanostructures. Porous silicon (PS) achieved by anodization of a highly doped silicon wafer offers oriented pores grown perpendicular to the surface and clearly separated from each other. Within the pores of the porous silicon matrix ferromagnetic nanostructures are precipitated. The obtained hybrid system merges the electronic properties of silicon with the magnetic properties of the incorporated ferromagnetic metal. On the one hand such a magnetic system can be achieved by electrochemical deposition of a transition metal from a metal salt solution into the pores of the nanostructured silicon skeleton. On the other hand magnetic particles of a few nanometers in size, fabricated in solution, can be incorporated by immersion. The electrochemically deposited nanostructures can be tuned in size, shape and their spatial distribution by the process parameters and thus specimens with desired ferromagnetic properties can be fabricated. Using magnetite nanoparticles for infiltration into porous silicon is not only of interest because of the magnetic properties of the composite material due to the possible modification of the ferromagnetic/superparamagnetic transition but also because of the biocompatibility of the system caused by the low toxicity of both materials. Thus it is a promising candidate for biomedical applications as drug delivery or biomedical targeting.

Introduction : Nanostructuring of materials results in a drastic change of their intrinsic properties. For example porous silicon achieved by anodization of a silicon wafer offers physical properties which can not be observed in case of bulk silicon. Microporous silicon which exhibits interconnected channels with diameters between 2 nm and 4 nm shows a strong luminescence in the visible [1] caused by quantum confinement effects. Macroporous silicon offers properties of a photonic crystal [2]. Moreover porous silicon possesses the ability to biodegrade within body fluids [3] and is known as a bioactive material [4], two properties

Proceeding of ICNM - 2009 1st International Conference on Nanostructured Materials and

Nanocomposites (6 – 8 April 2009, Kottayam, India)

Published by : Applied Science Innovations Private Limited, India. http://www.applied-science-innovations.com

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which play opposing roles. Both properties are of interest for medical applications as drug delivery [5] or tissue engineering [6]. Magnetic nanostructures play a crucial role in ferrofluids [7], high density magnetic data storage [8], catalysis [9] and also biomedical applications [10] for example as drug targeting. The fabrication of isolated magnetic nanoparticles is quite difficult to reach because the large surface areas oxidize easily when using metals. Furthermore they tend to agglomerate because of magnetic interactions. The monodisperse nanoparticles utilized in this work are prepared by high temperature decomposition of an organic precursor in the presence of oleic acid [11-13]. In the present work porous silicon templates with oriented pores are used to arrange magnetic nanostructures (electrodeposited or immersed) within a three-dimensional array by self-assembly. The combination of a semiconductor with magnetic materials leads to a hybrid system with specific magnetic properties but is also of interest for possible biomedical applications. The aim of the present work is to give an overview of the versatility of porous silicon and the advantage to combine this semiconductor material with a magnetic metal. Experimental results : The fabrication of PS is carried out by anodization of an n-type silicon wafer in aqueous hydrofluoric acid solution. Oriented growth and quasi-regular arrangement of the pores is achieved by adjusting the electrochemical parameters which is described in detail in a previous publication [14]. The achieved silicon templates are utilized on the one hand for electrochemical deposition of a ferromagnetic metal and on the other hand to infiltrate nanoparticles. The precipitation of metal-nanostructures by pulsed electrodeposition technique is performed in using an adequate metal salt solution [15]. The geometry and spatial distribution of the metal precipitates within the porous layer can be adjusted by the process parameters resulting in samples with tailored magnetic properties. Magnetite nanoparticles have been fabricated by high temperature decomposition of iron organic precursors following previously reported works [11, 12]. Particles of an average size of 9 nm have been obtained after performing the process steps described in [12]. These particles which have been mixed with hexane and oleic acid have been infiltrated by immersion into the pores of the porous silicon matrices. During this immersion process the temperature has been kept constant at room temperature. The immersion time has been typically 30 min. The two kinds of semiconductor/metal nanocomposites are characterized by electron microscopy (SEM, TEM) and magnetic measurements complement the investigations to figure out the different behaviour of the two types of specimens. The characterization of the porous silicon template regarding the pore-arrangement, porosity and pore-size as well as of the metal filled specimens with respect to the geometry and spatial distribution of the precipitated metal nanostructures is carried out by scanning electron microscopy (SEM). Figure 1 shows a cross-sectional survey of a typical porous silicon layer exhibiting straight pores grown perpendicular to the wafer surface with an average diameter of 55 nm. A top-view image of the quasi-regular pore-arrangement can be seen in the inset. Analysis of the top-view picture by image processing gives a porosity of about 60 %.

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Figure (1) : Scanning electron micrograph of the cross-section and the top-view (inset) of a porous silicon sample with a porosity of about 60% achieved by self-organization.

Precipitated metal nanostructures are investigated also by SEM in using the back scattered electrons to get element-sensitive information. Furthermore the nanocomposite is characterized by transmission electron microscopy (TEM) which allows to figure out the interfacial nature of the samples. Discussion :

Investigating the PS/metal interface by TEM one can say that the pore-walls of the PS-matrix are covered by an oxide layer of about 5 nm (figure 2). The oxidation of the pores is formed after the anodization by aging in air. FTIR-spectroscopy also shows the presence of oxide in case of aged porous silicon. The deposited metal (Ni) structures are also covered by oxide (figure 3) which likely arises after the preparation by focused ion beam. Magnetization measurements of Ni-filled samples do not show an exchange bias effect (not shown here) which indicates that the coverage of the nanostructures is not an antiferromagnetic Ni-oxide.

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Figure (2) : High resolution TEM image of porous silicon, showing an oxide layer of about 5 nm at the pore-walls.

Figure (3) : EELS line-scan over an embedded Ni-particle. Ni and oxygen has been identified, whereas the oxygen peak at the edges also originates from the oxygen covering the walls of the matrix because the two materials touch. Considering nanocomposites prepared by electrodeposition of a metal salt solution the specific metal precipitation which can be tuned by the electrochemical parameters and samples with desired magnetic properties can be achieved. Coercivities, magnetic remanence and magnetic anisotropy strongly depend on the geometry of the precipitated nanostructures as well as on their spatial distribution within the porous layer. Both features can be adjusted quite accurate mainly by varying the deposition current density and the frequency of the applied current. PS-matrices containing infiltrated magnetite nanoparticles form a composite material which is of interest due to the magnetic behaviour but also because of the biodegradability of both materials. This system shows superparamagnetic behaviour at room temperature and ferromagnetism at low temperatures. The transition between the two kinds of magnetism depends on the particle size but also on the interaction between the particles. The interaction between the nanoparticles can be influenced on the one hand by the thickness of the oleic acid coating and on the other hand by the concentration of the solution of the particles. Figure 4 shows the temperature dependent magnetization for two different concentrations of the particle solution. For decreasing concentration the blocking temperature TB is shifted to lower temperatures due to less interaction between the particles. In case of superparamagnetic, non-

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interacting particles of 9 nm in size TB can be estimated around 6 K in using the thermal energy

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2125 ⎟

⎞⎜⎝

⎛ −=K

HMKVTk CS

BBμ

, equ.1

being K the anisotropy constant, MS the saturation magnetization, HC the coercive field and V the volume of the individual particles. The measured TB at higher temperatures as well as the broad ZFC-peak are caused by magnetic interactions between the particles. Figure (4) : Zero field cooled/field cooled (ZFC/FC) measurements show a shift of the blocking temperature TB to lower temperatures with decreasing concentration which can be explained by less interaction between the particles. TB indicates the transition between ferro- and superparamagnetic behaviour. The broadening of the peak is not caused by inhomogeneous particle size distribution but by magnetic interactions between the particles. Conclusion :

Porous silicon is a versatile material applicable in many fields of nano-research. In the present work it is used as template material to embed magnetic nanostructures. On the one hand ferromagnetic metals are electrochemically deposited within the pores leading to a nanocomposite material which is of interest because of the silicon base material and the adjustability of the ferromagnetic properties. On the other hand Fe3O4-nanoparticles are infiltrated within the porous layer. The latter system exhibits ferro-/superparamagnetic properties which can be influenced but it is also a promising candidate for biomedical applications as drug delivery and drug targeting. All in all porous silicon/metal composites are of great interest in basic research but they are also of interest for various magnetic and biomedical applications. Acknowledgements :

This work is supported by the Austrian FWF under project P 21155. The authors would like to thank M.P. Morales and A.G. Roca of the Instituto de Ciencia de Materiales de Madrid,

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CSIC for the preparation of magnetite nanoparticles and Prof. H. Krenn from the Institute of Physics at the Karl Franzens Universiy Graz to make available the SQUID-magnetometer. References :

[1] L. T. Canham, Applied Physic Letters, 57, 1046 (1990). [2] K. Busch, S. Lölkes, R. B. Wehrspohn, H. Föll, Photonic crystals: Advances in design, fabrication ans characterization, Wiley-VCH, Berlin 2004. [3] L. Canham, Advanced Materials, 7, 1033 (1995). [4] L. T. Canham, C. L. Reeves, D. O. King, P. J. Branfield, J. G. Crabb, M. C. L. Ward, Adv. Mater. 8, 850 (1996). [5] L. T. Canham, Nanotechnology 18, 185704 (2007). [6] W. Sun, J. E. Puzas, T.-J. Sheu, Ph. M. Fauchet, Phys. Stat. Sol. (a) 204, 1429 (2007). [7] J. Park, K. An, Y. Hwang, J. G. Park, H. J. Noh, J. Y. Kim, J. H. Park, N. M. Hwang, T. Hyeon, Nature Materials 3, 891 (2004). [8] Ch. S. Gill, B. A. Price, Ch. W. Jones, Journal of Catalysis 251, 145 (2007). [9] G. Reiss, A. Huetten, Nature Materials 4, 725 (2005). [10] P. Tartaj, M. P. Morales, T. Gonzalez-Carreno, S. Veintemillas-Verdaguer, C. J. Serna, J. Mag. Mag. Mat. 290-291, 28 (2005). [11] T. Hyeon, S. S. Lee, J. Park, Y. Chang, H. B. Na, J. Am. Chem. Soc. 123, 12798 (2001). [12] S. Sun, H. J. Zeng, Am. Chem. Soc, 124, 8204 (2002). [13] W. W. Yu, J. C. Falkner, C. T. Yavuz, V. L. Colvin, Chem. Commun. 20, 2306 (2004). [14] P. Granitzer, K. Rumpf, P. Pölt, A. Reichmann, H. Krenn, Physica E 38, 205 (2007). [15] P. Granitzer, K. Rumpf, P. Poelt, S. Simic, H. Krenn, Phys. Stat. Sol. (a) 205, 1443 (2008).