Type of presentation: Poster

MS-5-P-2639 The modulated structure of Fe2O3(ZnO)7 studied by HAADF-STEM

Eichhorn S.1, Schmid H. K.1,2, Mader W.1
1Inst. Inorganic Chemistry, University Bonn, Bonn, Germany, 2now with JEOL (Germany) GmbH, Eching, Germany
mader@uni-bonn.de

The existence of phases ABO3(ZnO)m in the system ZnO-Fe2O3 is known up to a composition of Fe2O3(ZnO)12 at 1350 °C [1]. These phases share the structural characteristics of the better known compounds InFeO3(ZnO)m [2] which exist in the range m ≥ 1. ABO3(ZnO)m compounds consist of wurtzite slabs separated by layers of AO6 octahedrons fully occupied by A3+ cations such as In3+. Within the wurtzite layers B3+ ions occupy tetrahedral positions. The crystal structures of compounds with low ZnO content were verified by single crystal X-ray diffraction [3], however Fe2O3(ZnO)m compounds show an obvious super-structure in diffraction.
We obtained Fe2O3(ZnO)7 by solid state reaction of ZnO and ZnFe2O4 powders at 1600 °C. The reaction product was quenched in water to retain the metastable high temperature phase. XRD proves the layer structure of Fe2O3(ZnO)7, however, EDS measurements show a metal content of 30% Fe and 70% Zn vs. nominal composition of 22% Fe and 78% Zn as derived from the formula. Hence, the correct formula should be written as Fe2O3(Zn1-xFexO)7 with x ≈ 0.1. The Compound crystallizes in the monoclinic system with lattice constants a = 5.566(8) Å, b = 3.234(5) Å, c = 24.00(3) Å and β = 95.35° with possible spacegroups C2, Cm or C2/m. EDS and electron diffraction was conducted on a Philips CM30 with a Noran System 7 EDS system and a twin lens providing large tilt angles of up to 45°. HAADF was conducted on a probe Cs-corrected JEOL ARM200F equipped with a cold FEG.
Figure 1 shows an SAED pattern from Fe2O3(ZnO)7 in [100] orientation where additional superstructure reflections 0klx are clearly visible as satellites to the main reflections. The modulation vector q is about 34 Å measured from electron diffraction patterns. The periodicity of the (00l) reflections corresponds to a 24 Å lattice plane spacing.
A HAADF micrograph in the same orientation is shown in figure 2. Multiple layers of Zn2+ cations show a wave like modulation along [010] direction. Also Fe3+ octahedral layers show considerably less detail in atomic resolution which is attributed to significant displacements of Fe3+ cations in FeO6-octahedrons. The misfit of the rather small Fe3+ cation in octahedral coordination is considered to be the origin of the structure modulation.
These materials offer challenging crystallographic and analytical questions, such as Fe2+ distribution in the wurtzite layers, which can be tackled by advanced electron microscopy methods, i.e. quantitative EDS and EELS analyses with high spatial resolution in TEM/STEM [4].

[1] N. Kimizuka et al., J. Solid State Chem. 103 (1993) p. 394
[2] N. Kimizuka et al., J. Solid State Chem. 74 (1988) p. 98
[3] I. Keller et al., Z. Anorg. Allg. Chem. 635 (2009) p. 2065
[4] H. Schmid et al., Ultramicroscopy. 127 (2013) 76-84


Fig. 1: SAED pattern of Fe2O3(Zn1-xFexO)7 in [100]. Periodicity of <00l>reflections is 24 Å, of <0k0> reflections is 34 Å.

Fig. 2: HAADF STEM micrograph of Fe2O3(Zn1-xFexO)7 in [100] orientation. Layers of FeO6-octahedrons are marked by arrows.