Abstract

Reduced terminations of the Fe${}_{3}$O${}_{4}$(001) surface were studied using scanning tunneling microscopy, x-ray photoelectron spectroscopy (XPS), and density functional theory (DFT). Fe atoms, deposited onto the thermodynamically stable, distorted B-layer termination at room temperature (RT), occupy one of two available tetrahedrally coordinated sites per ($\sqrt{2}\ifmmode\times\else\texttimes\fi{}\sqrt{2}$)$R$45\ifmmode^\circ\else\textdegree\fi{} unit cell. Further RT deposition results in Fe clusters. With mild annealing, a second Fe adatom per unit cell is accommodated, though not in the second tetrahedral site. Rather both Fe atoms reside in octahedral coordinated sites, leading to a ``Fe-dimer'' termination. At four additional Fe atoms per unit cell, all surface octahedral sites are occupied, resulting in a FeO(001)-like phase. The observed configurations are consistent with the calculated surface phase diagram. Both XPS and DFT+$U$ results indicate a progressive reduction of surface iron from Fe${}^{3+}$ to Fe${}^{2+}$ upon Fe deposition. The antiferromagnetic FeO layer on top of ferromagnetic Fe${}_{3}$O${}_{4}$(001) suggests possible exchange bias in this system.

Highlights

  • Iron, the fourth most abundant element in the Earth’s crust, is oxidized under ambient conditions forming several stable Fe oxides and hydroxides.1 The Fe oxides differ in the concentration, distribution, and oxidation state of Fe cations in interstitial sites of a close-packed oxygen anion lattice.1 Under oxidizing conditions, hematite (α-Fe2O3) and maghemite (γ -Fe2O3) are stable phases; Fe3+ occupy both octahedral (Fe-O6) and tetrahedral (Fe-O4) coordinated sites in maghemite, and octahedral sites in hematite

  • Over a broad range of oxygen chemical potentials the phase diagram is dominated by the distorted B-layer termination [see Fig. 1(b)], as reported previously

  • Towards the Fe-rich limit, the density functional theory (DFT) calculations show that our model of the 1 ML Fe-dimer termination is energetically favorable over a 1 ML FeA termination

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Summary

Introduction

The fourth most abundant element in the Earth’s crust, is oxidized under ambient conditions forming several stable Fe oxides and hydroxides. The Fe oxides differ in the concentration, distribution, and oxidation state of Fe cations in interstitial sites of a close-packed oxygen anion lattice. Under oxidizing conditions, hematite (α-Fe2O3) and maghemite (γ -Fe2O3) are stable phases; Fe3+ occupy both octahedral (Fe-O6) and tetrahedral (Fe-O4) coordinated sites in maghemite, and octahedral sites in hematite. Hematite (α-Fe2O3) and maghemite (γ -Fe2O3) are stable phases; Fe3+ occupy both octahedral (Fe-O6) and tetrahedral (Fe-O4) coordinated sites in maghemite, and octahedral sites in hematite. Under reducing conditions wustite (FeO) is formed, in which Fe2+ cations occupy octahedral coordinated sites. Magnetite (Fe3O4) represents the stable intermediate case, with both Fe3+ and Fe2+ cations present in an inversespinel structure [standard formula AB2O4; see Fig. 1(a)]. Fe3+ cations (denoted FeA; blue in Fig. 1) occupy one-eighth of the tetrahedral sites, while a 1:1 mixture of Fe2+ and Fe3+ fills half of the octahedral sites (FeB, yellow). The mixed valence of Fe3O4 leads to several interesting and useful phenomena including ferrimagnetism and redox surface chemistry, while band structure calculations predict room-temperature halfmetallicity.. The mixed valence of Fe3O4 leads to several interesting and useful phenomena including ferrimagnetism and redox surface chemistry, while band structure calculations predict room-temperature halfmetallicity. The surface properties play an important role in many applications including geochemistry, corrosion science, weathering, biomedicine, and heterogeneous catalysis.

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