Abstract

We here report an investigation of the electronic states in the $R\mathrm{F}{\mathrm{e}}_{2}{\mathrm{O}}_{4}(R=\mathrm{Lu},\phantom{\rule{0.16em}{0ex}}\mathrm{Yb},\phantom{\rule{0.16em}{0ex}}\mathrm{Tm},\phantom{\rule{0.16em}{0ex}}\mathrm{Y})$ mixed-valence ferrites by means of soft x-ray absorption spectroscopy (XAS) and x-ray magnetic circular dichroism (XMCD) measurements together with ab initio theoretical calculations. The presence of ${\mathrm{Fe}}^{+2}$ and ${\mathrm{Fe}}^{+3}$ pure ionic species is discarded in the XAS spectra at the $\mathrm{O}\phantom{\rule{0.16em}{0ex}}K$ edge in both experimental data and simulations based on the multiple scattering theory. Similarly, no trace of $\mathrm{F}{\mathrm{e}}^{+2}/\mathrm{F}{\mathrm{e}}^{+3}$ contributions is detected in the XMCD spectra at the $\mathrm{Fe}\phantom{\rule{0.16em}{0ex}}K$ edge. On the other hand, the XAS and XMCD spectra at the $\mathrm{Fe}\phantom{\rule{0.16em}{0ex}}{L}_{2,3}$ edges can be well described in terms of $\mathrm{F}{\mathrm{e}}^{+2}/\mathrm{F}{\mathrm{e}}^{+3}$ contributions, and are also supported by multiplet calculations. This finding can be interpreted as the existence of a mixture of $3{d}^{5}/3{d}^{6}$ configurations at the Fe atoms. Alternative ferrimagnetic spin orderings based on a trimodal Fe valence distribution are also proposed and discussed. Finally, a possible explanation for the strong dependence of the $\mathrm{Fe}\phantom{\rule{0.16em}{0ex}}{L}_{2,3}$ edges XMCD signal magnitude on both the sample surface preparation and detection method is presented.

Highlights

  • Mixed-valence transition-metal oxides exhibit remarkable properties such as high temperature superconductivity, colossal magnetoresistance, and multiferroicity, which may give rise to important technological applications [1]

  • Fe+2/Fe+3 charge ordering (CO) leading to a polar configuration in LuFe2O4 lacks experimental support. These results suggest that the Fe atoms in the mixed-valence RFe2O4 compounds are in a homogeneous mixed-valence state instead of a heterogeneous mixed-valence state between two integer valences

  • This investigation adds to other recent published papers [10,38,39,40,41,42,43,44] to provide a framework for the physics of the mixed-valence RFe2O4 (R = Lu, Yb, Tm, Y) compounds, which in some aspects can be extended to other mixed-valence oxides

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Summary

INTRODUCTION

Mixed-valence transition-metal oxides exhibit remarkable properties such as high temperature superconductivity, colossal magnetoresistance, and multiferroicity, which may give rise to important technological applications [1]. Previous to these recent results, various x-ray magnetic circular dichroism (XMCD) experiments at the Fe L2,3 edges in LuFe2O4 [27,30,38] were interpreted using a spin ordering model in terms of the Fe+2/Fe+3 ionic species in which all Fe+2 as well as 1/3 of the Fe+3 moments are aligned parallel to the applied magnetic field and the remaining 2/3 of the Fe+3 in an antiparallel way In view of these results, a consistent description of the local electronic and magnetic structure of the RFe2O4 compounds in the new framework of homogeneous intermediate valence state for the Fe atoms is mandatory.

EXPERIMENTAL AND CALCULATION DETAILS
XANES at the O K edge
XMCD at the Fe K edge
DISCUSSION AND CONCLUSIONS
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