Abstract

The crystal structure of the Sb6O13 oxide, exhibiting a defect pyrochlore crystal structure with atomic vacancies, has been studied using a complete set of state-of-the-art techniques. The degree of antimony disproportionation in Sb3+ and Sb5+ valence states has been directly determined around 36% and 64%, respectively, using X-ray absorption near edge structure (XANES). These findings are in excellent agreement with our Rietveld analysis of synchrotron X-ray (SXRD) and neutron powder diffraction (NPD) results. Moreover, the highly distorted Sb3+ coordination due to its lone electron pair has been critically revisited. The bonding distances and coordination of Sb3+ and Sb5+ species closely agree with an extensive dynamic and crystallographic determination using the Extended X-ray Absorption Fine Structure (EXAFS) technique. Most importantly, the specific local disorder of the two distinctive Sb ions has been crosschecked monitoring their unusual Debye–Waller factors.

Highlights

  • The crystal structure of the ­Sb6O13 oxide, exhibiting a defect pyrochlore crystal structure with atomic vacancies, has been studied using a complete set of state-of-the-art techniques

  • A Fourier difference density map performed from neutron powder diffraction (NPD) data, collected at room temperature (RT), led to negative scattering density at 8a position and a positive density dispersed in its vicinity, as shown in Supplementary Fig. S2

  • The complementary structural and dynamic study of ­Sb6O13 using long- and short-range diffraction techniques together with X-ray Absorption Fine Spectroscopy confirms that this particular Sb-oxide can be precisely described as a defect pyrochlore, defined in the Fd3m space group

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Summary

Introduction

The crystal structure of the ­Sb6O13 oxide, exhibiting a defect pyrochlore crystal structure with atomic vacancies, has been studied using a complete set of state-of-the-art techniques. The broad family of pyrochlore oxides, with the general formula A2B2O6O′(space group: Fd3m , Z = 8) displays an incomparable flexibility, concerning cationic substitutions, atomic vacancies, structural defects, and related superstructures, accounting for the wide panoply of physical properties and a­ pplications[8], including thermal, electrical, and magnetic properties. They have shown high resistance to radiation damage and temperature, and improved catalytic effects on water ­splitting[9,10,11,12]. The free space of the above (B2O6) framework can be filled with a second framework related to the (A2O′) units, or with separate individual ions and/or H­ 2O molecules

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