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Wide-angle X-ray scattering and Reverse Monte Carlo studies of Fe80B20, Co80B20, Mg60Cu30Y10 metallic glasses A

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KSUPS 2015: Abstracts / Extended abstracts / Synchrotron Radiation in Natural Science Vol. 14, No. 1-2 (2015)

8

L-04 Tue. 01. 09., 1500-1540

Wide-angle X-ray scattering and Reverse Monte Carlo studies of Fe80B20, Co80B20, Mg60Cu30Y10

metallic glasses

A. Burian1,2*, R. Babilas3, A. Fitch4, L. Temleitner5

1A. Chełkowski Institute of Physics, University of Silesia, ul.

Uniwersutecka 4, 40-007 Katowice, Poland

2Silesian Center of Education and Interdisciplinary Research, ul. 75 Pułku Piechoty, 40-500 Chorzów, Poland

3Institute of Engineering Materials and Biomaterials, Silesian University of Technology, ul. Konarskiego 18a, 44-100 Gliwice, Poalnd

4European Synchrotron Radiation Facility, B.P.220, F-38043 Grenoble Cedex, France

5Institute for Solid State Physics and Optics, Wigner Research Centre for Physics, Hungarian Academy of Sciences, PO Box 49, H-1525 Budapest, Hungary

Keywords: synchrotron radiation, metallic glasses, wide-angle X-ray scattering, Reverse Monte Carlo

*e-mail: andrzej.burian@us.edu.pl

The atomic scale structure of Fe80B20, Co80B20 and Mg60Cu30Y10 metallic glasses has been studied using the wide-angle X-ray scattering and reverse Monte Carlo methods. The Fe80B20 and Co80B20 samples were prepared in the form of amorphous ribbons with thickness of 0.03 mm and width of 5 mm by the “chill- block melt spinning technique under the argon protective atmosphere. The bulk Mg60Cu30Y10 glass was obtained by injection of the Mg-Cu-Y melted material in the proportion 60:30:10 into a copper mold by a pressure casting method.

The wide-angle X-ray scattering measurements were performed on the ID31 beam-line at the European Synchrotron Radiation Facility, Grenoble, France. The incident beam energy of 31 keV yielding the wavelength of 0.4 Å was used in this experiment. The scattered intensities were recorded to the maximum value of the

scattering vector Q=4πsinθ/λ = 23 Å-1, where 2θ is the scattering angle and λ is the wavelength.

As the atomic scale structure of the investigated materials cannot be described using formalism of crystallography an approach based on the Reverse Monte Carlo [1] fitting procedure was used. In this method Marcov chain sampling with the Metropolis accelerating algorithm [2] allows generation of three dimensional particle configuration that is consistent with the experimentally measured structure factor. The fit quality is evaluated by a standard χ2 test in which the experimental errors are taken into account.

In our previous paper [3] the local atomic arrangement in the Fe80B20 glass was compared with those of the Fe3B, Fe23B6 and bcc Fe crystalline phases.

From this comparison it has been concluded that the local structure of the crystalline counterparts is not consistent with the experimental data for glassy Fe80B20.

The Reverse Monte Carlo method applied for the Fe80B20, Co80B20 and Mg60Cu30Y10 metallic glasses allowed obtaining perfect fit to the experimental structure factors and to the experimental pair distribution functions. Resemblance of the local structure, which extends up to approximately 20 Å, to the icosahedral and trigonal prism configurations is discussed. The Reverse Monte Carlo results are compared with high-resolution transmission electron microscopy observations. From this comparison it can be concluded that both methods lead to consistent description of the local atomic arrangement in the investigated materials.

Acknowledgments: This work was supported by the National Science Centre under the research project No.:

2011/03/D/ST8/04138.

___________________________________________________

[1] R. L. McGreevy and L. Pusztai, Molecular Simulation 1 (1988) 359.

[2] N. Metropolis, A.W. Rosenbluth, M.N. Rosenbluth, A.H. Teller, E. Teller, J. Chem. Phys. 21 (1953) 1087.

[3] R. Babilas, Ł. Hawełek, A. Burian, J. Solid State Chemistry 219 (2014) 179.

[4] R. Babilas, R. Nowosielski, M. Pawlyta, A. Fitch, A. Burian, Materials Characterization, in press.

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