Effect of synthesis method on the ferromagnetic behavior ZnO nanoparticles MdGazzali P.M.*, SoumyaRajan, G.Chandrasekaran Department of Physics, Pondicherry University, R. Venkataraman Nagar, Kalapet, Pondicherry-605014, India * Corresponding author’s e-mail:gazzali313@gmail.com, Tel.: +91-9444905538 ℎ𝑖𝑔ℎ Abstract We report a comparative study of chemically synthesized and ball milled ZnO in order to understand the role of defects and lattice strain. Important conclusion has been drawn from the results of structural, optical and magnetic studies. Keywords: Nanoparticles, autocombustion. XRD, VSM bill-milling, sol-gel Introduction ZnO has attracted considerable attention as a semiconducting material with wide direct band gap and large exciton binding energy at room temperature. Extensive research on ZnO confirmed that it is a proper candidate to be used in the field of electronics, gas sensors,photovoltaics, electrochemistry and thin film transistors. The various properties of ZnO depend on the composition and morphology and defect structure [1]. It is well known that the oxygen vacancies affect the properties of ZnO significantly. In this work we applied XRD, Raman and UV measurements to study the defect induced ferromagnetism in mechanically activated and chemically prepared samples. Experimental The commercial ZnO powder (Himedia A.R. 99.5 %) is mechanically milled in a planetary ball mill for two different milling times, 150 and 300 minutes and designated as bulk, ZnO-150 and ZnO-300. ZnO NPs are also prepared by sol-gel auto-combustion method with zinc nitrate and glycine as precursors and designated as ZnO-CM. The phase identification of the samples is determined using X’Pert PRO X-ray Diffractometer with Cu-Kα radiation. Raman scattering measurements are recorded using confocal microRaman microscope (Renishaw inVia Reflex) in the range 100–1400 cm-1 with an excitation wavelength of 514.5 nm. Room temperature M-H loop measurements are carried out using Vibrating Sample Magnetometer (Lakeshore VSM 7410). UV-Vis absorption / reflectance measurements are made by Lambda 650 UV-Vis diffuse reflectance spectrometer (PerkinElmer). Results and discussions X-Ray diffraction patterns all the samples are coinciding with the peaks of ZnO wurtzite structure (JCPDS No: 01-075-0576). Particle size, lattice strain and lattice constants are calculated. The observed shift and enhancement of FWHM of 𝐸2 ~ 438 cm-1 and E1(LO) ~ 586 cm-1 phonon modes in the Raman spectra may be attributed to the increased defect density concentration and lattice strain [2]. UV studies show a decrease in band gap energy (Eg) with the lowest value (3.21 eV) for the ZnO-150 sample.The observed red shift of Eg may be induced by electrons generated from oxygen vacancies [3]. VSM measurements confirm the soft ferromagnetic (FM) nature in all the samples. Magnetization is found to increase with the increase in milling time. But the ZnO-CM shows the highest magnetization of 126 memu/g and coercivity of 141 Oe among our samples. This controversy may be attributed to the presence of residual carbon in the chemically prepared ZnO lattice [4]. Conclusion The structural characterization of the starting ZnO powder and its variation upon by mechanical activation and chemical preparation are performed by XRD and Raman scattering measurements. The band gap energy variation of the samples reflects the impact of intrinsic and extrinsic defects. The occurrence of oxygen vacancies induces FM in the investigated samples. Reference [1] V. Ischenko, S. Polarz, D. Grote, V. Stavarachem, K. Fink, and M. Driess, “Zinc Oxide Nanoparticles with Defects” Adv. Funct. Mater., 15, 12, (2005), pp. 1945 1954. [2] K. Vojisavljević, M. Šćepanović, T. Sreckovic, M. G. Brojčin, Z. Brankovic, and G. Brankovic, “Structural characterization of mechanically milled ZnO: influence of zirconia milling media”, J. Phys.: Condens. Matter, 20, 47, (2008), pp. 475202-4752011. [3] M. Suchea, S. Christoulakis, N. Katsarakis, T. Kitsopoulos, and G. Kiriakidis, “Comparative study of zinc oxide and aluminum doped zinc oxide transparent thin films grown by direct current magnetron sputtering”, Thin Solid Films, 515, 16, (2007), pp. 65626566. [4] H. Pan, J. B. Yi, L. Shen, R. Q. Wu, J. H. Yang, J.Y. Lin, Y. P. Feng, J. Ding, L. H. Van, and J. H. Yin,“Room-Temperature Ferromagnetism in CarbonDoped ZnO”, Phys. Rev. Lett., 99, 12, (2007), pp. 127201-127204.