Magnetic structure and transport properties of Ba2FeWO6 synthesized in ambient H2: Ar gas Jasnamol P P*, Neenu Lekshmi P, Manoj Raama Varma CSIR-National Institute for Interdisciplinary Science and technology, Trivandrum, India * jasnayasbe@gmail.com, Tel.: +91-471-2515377 Abstract Synthesized Ba2FeWO6 with cubic crystal structure in ambient H2: Ar gas. Magnetic structure is to be accredited with characterization using magnetic susceptibility as a function of temperature and applied magnetic field. Transport properties of Ba2FeWO6 will also be presented. account of the recent focus on spintronics application of double perovskite materials. Keywords: A2BB’O6, Double-perovskite, Magnetic structure, Spintronics, Transport properties. Introduction The discovery of the large room temperature magnetoresistance in double-perovskite Sr2FeMoO6 with Tc around 420K [1] has entertained researcher’s focus on double perovskite materials A2BB’O6 with A being alkaline earth metal or rare earth element, B and B’ being transition metals. In 1959, E. J. Fresia et al. synthesized Ba2FeWO6 (BFWO) and identified cubic crystal structure [2]. Later in 2002, A. K. Azad et al. reported BFWO with tetragonal I4/m crystal structure [3] and an antiferromagnetic ordering below 30K [4]. In 2004, N. Rammeh et al. reported the BFWO having cubic Fm-3m crystal structure [5] with antiferromagnetic ordering. The present study investigates the magnetic structure and the transport properties of BFWO synthesized with ambient H2: Ar mixture gas, where the up to day results on this topic are all on materials synthesized in air atmosphere [1-4] or in evacuated silica tube [5]. High purity BaCO3, Fe2O3 and WO3 are used as the starting materials to synthesize BFWO through standard solid state reaction route. The pre-calcinated powders are sintered with 9% H2: Ar gas as surrounding atmosphere. The X ray diffraction pattern is obtained and is identical to cubic Fm-3m structure, same as that reported by N. Rammeh et al. [5], synthesized in evacuated silica tube. The magnetic structure of the as synthesized BFWO will be identified by Susceptibility vs. temperature and Magnetization vs. applied magnetic field plot. The transport properties are also studied on Fig. 1: XRD pattern of Ba2FeWO6 Acknowledgment The authors acknowledge Department of Science and Technology, University Grand Commission and Council of Scientific and Industrial Research, Gov. of India for funding and fellowship. References [1] K.-I. Kobayashi, T. Kimura, H. Sawada, K. Terakura, and Y. Tokura, “Room-temperature magnetoresistance in an oxide material with an ordered double-perovskite structure”, Nature, 395, 15 October, (1988), pp. 677-680. [2] E. J. Fresia, Lewis Katz, and Roland Ward, “Cation Suubstitution in Perovskite-like Phases”, J. Am. Chem. Soc., 81, (1959), pp. 4783-4785. [3] A.K. Azad, A. Mellergård, S.G. Eriksson, S.A. Ivanov, J. Eriksen, H. Rundlöf, “Preparation, crystal and magnetic structure of the double perovskite Ba2FeWO6”, Appl. Phys. A, 74, (2002), pp. S763–S765. [4] A.K. Azad, S.G. Eriksson, A. Mellergård, S.A. Ivanov, J. Eriksen, H. Rundlöf,, “A study on the nuclear and magnetic structure of the double perovskites A2FeWO6 (A=Sr, Ba) by neutron powder diffraction and reverse Monte Carlo modeling”, Materials Research Bulletin, 37, (2002), pp. 1797-1813. [5] N. Rammeh, K.G. Bramnik, H. Ehrenberg, B. Stahl, H. Fuess, A. Cheikh-Rouhou, “Crystal structure and magnetic properties of Mo-substituted ‘Ba2(Fe,W)2O6’ double-perovskites: a synchrotron diffraction, magnetization and Mössbauer study”, Journal of Alloys and Compounds, 363, (2004), pp. 24– 31.