Abstract

Ferrihydrite is one of the most important iron-containing minerals on Earth. Yet determination of its atomic-scale structure has been frustrated by its intrinsically poor crystallinity. The key difficulty is that physically-different models can appear consistent with the same experimental data. Using X-ray total scattering and a nancomposite reverse Monte Carlo approach, we evaluate the two principal contending models—one a multi-phase system without tetrahedral iron(III), and the other a single phase with tetrahedral iron(III). Our methodology is unique in considering explicitly the complex nanocomposite structure the material adopts: namely, crystalline domains embedded in a poorly-ordered matrix. The multi-phase model requires unphysical structural rearrangements to fit the data, whereas the single-phase model accounts for the data straightforwardly. Hence the latter provides the more accurate description of the short- and intermediate-range order of ferrihydrite. We discuss how this approach might allow experiment-driven (in)validation of complex models for important nanostructured phases beyond ferrihydrite.

Highlights

  • Ferrihydrite is one of the most important iron-containing minerals on Earth

  • We begin with a brief description of our approach for generating atomistic representations of ferrihydrite for subsequent reverse Monte Carlo (RMC) analysis; full details are provided in the Supplementary Methods

  • Individual nanoparticles are positioned and oriented randomly within the final box; at this stage we aim for a filling ratio of ~50%, achieved using a hard-sphere Monte Carlo (MC) algorithm

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Summary

Introduction

Ferrihydrite is one of the most important iron-containing minerals on Earth. Yet determination of its atomic-scale structure has been frustrated by its intrinsically poor crystallinity. The multi-phase model requires unphysical structural rearrangements to fit the data, whereas the single-phase model accounts for the data straightforwardly The latter provides the more accurate description of the short- and intermediate-range order of ferrihydrite. Approach is to approximate nanomaterials as periodic crystals modified by a suitable shape function This interpretation is implicit in Debye–Sherrer analysis of diffraction peak widths but is sometimes carried out explicitly via modelling of the pair distribution function (PDF) with appropriate damping functions[18,19]. The difficulty in all comparative studies is that the MP model requires significant simplifications[26] to allow its complex composition to be approximated by a single damped periodic structure

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