Radiation-Induced Solid-State Transformations of Uranyl Peroxides

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Abstract

Single-crystal X-ray diffraction studies of pristine and γ-irradiated Ca2[UO2(O2)3]·9H2O reveal site-specific atomic-scale changes during the solid-state progression from a crystalline to X-ray amorphous state with increasing dose. Following γ-irradiation to 1, 1.5, and 2 MGy, the peroxide group not bonded to Ca2+ is progressively replaced by two hydroxyl groups separated by 2.7 Å (with minor changes in the unit cell), whereas the peroxide groups bonded to Ca2+ cations are largely unaffected by irradiation prior to amorphization, which occurs by a dose of 3 MGy. The conversion of peroxide to hydroxyl occurs through interaction of neighboring lattice H2O molecules and ionization of the peroxide O-O bond, which produces two hydroxyls, and allows isolation of the important monomer building block, UO2(O2)2(OH)24-, that is ubiquitous in uranyl capsule polyoxometalates. Steric crowding in the equatorial plane of the uranyl ion develops and promotes transformation to an amorphous phase. In contrast, γ-irradiation of solid Li4[(UO2)(O2)3]·10H2O results in a solid-state transformation to a well-crystallized peroxide-free uranyl oxyhydrate containing sheets of equatorial edge and vertex-sharing uranyl pentagonal bipyramids with likely Li and H2O in interlayer positions. The irradiation products of these two uranyl triperoxide monomers are compared via X-ray diffraction (single-crystal and powder) and Raman spectroscopy, with a focus on the influence of the Li+ and Ca2+ countercations. Highly hydratable and mobile Li+ yields to uranyl hydrolysis reactions, while Ca2+ provides lattice rigidity, allowing observation of the first steps of radiation-promoted transformation of uranyl triperoxide.

Original languageEnglish
Pages (from-to)882-889
Number of pages8
JournalInorganic Chemistry
Volume61
Issue number2
DOIs
StatePublished - Jan 17 2022
Externally publishedYes

Funding

This research was supported by the Department of Energy, National Nuclear Security Administration, under Award Number DE-NA0003763. D.E.F. and P.C.B. were funded under this award until December 2020 and then by other University funds. The authors thank Bryan E. Galeas for synthetic efforts. The authors acknowledge the Center for Sustainable Energy at Notre Dame (ND Energy) Materials Characterization Facilities for the use of the Bruker D8 Advance Davinci Powder X-ray Diffractometer. The authors thank Prof. Ian Carmichael for making available the facilities of the Notre Dame Radiation Laboratory, which is supported by DOE BES through grant number DE-FC02-04ER15533. This contribution is NDRL-5317 from the Notre Dame Radiation Laboratory.

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