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Struktur und Dynamik Poster: Mi., 14:00–16:30 M-P138<br />

Na2O - Fe2O3 - SiO2 glasses: Inhomogeneous distribution of Fe in channels<br />

Florian Kargl 1,2 , Andreas Meyer 2 , Michael Marek Koza 3<br />

1 Department of Applied Science, Chalmers University of Technology, 41296 Göteborg,<br />

Schweden – 2 <strong>Deutsche</strong>s Zentrum für Luft und Raumfahrt, Institut für Raumsimulation,<br />

51170 Köln – 3 Institute Laue-Langevin, 38042 Grenoble, Frankreich<br />

We report on the investigation of ternary sodium iron-silicate glasses by means of neutron<br />

spectroscopy and diffraction. Being of outstanding importance for geosciences,<br />

iron bearing silicate glasses and melts show a number of unique features [1]. Adding<br />

Fe2O3 to a binary alkali silicate melt leads to an increase in melt viscosity. This increase<br />

depends not only on the amount of Fe2O3, but also on the conditions of synthesis.<br />

For instance, under normal conditions of synthesis Fe is predominantly built into the<br />

structure as Fe 3+ . Depending on melt composition, temperature, and atmosphere Fe<br />

can also exist in the reduced form Fe 2+ .<br />

We demonstrate that a partial Fe-Fe structure factor can be directly obtained in these<br />

multicomponent system. Neutrons scattered on Fe 3+ couple to its unpaired electron<br />

spin moment. Quasielastic neutron scattering allows to separate nuclear from magnetic<br />

scattering contributions in sodium iron silicates. The results were corroborated by<br />

experiments using polarization analysis. The partial Fe-Fe structure factor determined<br />

by means of magnetic scattering features a correlation peak around 0.9 ˚A −1 . A<br />

correlation peak in the nuclear elastic structure factor observed at the same position<br />

in binary alkali silicate melts was shown to reflect a network of percolation channels<br />

for fast alkali ion diffusion [2]. The addition of a second network forming component,<br />

Al2O3, leads to a drastic increase in viscosity and a disruption of the channel structure.<br />

This is evidenced by vanishing of this correlation peak in the nuclear elastic structure<br />

factor [3]. Considering the total nuclear structure factor consisting of ten different<br />

partial structure factors the position of Al with respect to the other components cannot<br />

be unambiguously determined. In the sodium iron-silicates the position of the correlation<br />

peak is Fe concentration independent. However, the peak height scales with the<br />

total Fe3+ content. The experiments indicate an inhomogeneous distribution of Fe.<br />

They further suggest that the Fe atoms are located on Na equivalent positions rather<br />

than on those equivalent to Si.<br />

[1] Y. Bottinga, D. B. Dingwell, and P. Richet, edts., 6th Silicate Melt Workshop,<br />

Chem. Geol. 174, (2001) 1; Y. Bottinga, D. B. Dingwell, P. Richet, and M. Toplis<br />

edts., 7th Silicate Melt Workshop, Chem. Geol. 213, (2004) 1.<br />

[2] A. Meyer, J. Horbach, W. Kob, F. Kargl, and H. Schober, Phys. Rev. Lett. 93,<br />

(2004) 027801.<br />

[3] F. Kargl and A. Meyer, Chem. Geol. 213, (2004) 165.

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