Irradiation-enhanced Interactions at UO2/Al2O3/Al Interfaces

  • Stefania Dede
  • , Khachatur V. Manukyan
  • , Jordan M. Roach
  • , Daniel Robertson
  • , Peter C. Burns
  • , Ani Aprahamian

Research output: Contribution to journalArticlepeer-review

1 Scopus citations

Abstract

Combustion synthesis is used to prepare thin UO2 films on aluminum alloy substrates. This simple preparation method involves electrospraying uranyl nitrate + acetylacetone + 2-methoxyethanol solution on the substrate, followed by a short annealing at 350 or 550 °C. The irradiation of films with a 40Ar2+ ion beam (energy of 1.7 MeV and fluences of 7.7 × 1016 and 1.3 × 1017 ions/cm2) is conducted to investigate irradiation-induced restructuring processes. High-resolution transmission electron microscopy (TEM) and X-ray photoelectron spectroscopy (XPS) investigations show that the annealing temperature significantly influences the crystallinity and stability of materials during irradiation. A small amount of Mg in the alloy substrate diffuses into the amorphous Al2O3 interfacial layer between the film and the substrate. Local thermal spikes from the incoming ions facilitate the irradiation-induced mixing of immiscible Al2O3 and UO2 for the materials prepared at 350 °C. This mass diffusion produces relatively large cavities at the interface. Selective diffusion of a more significant amount of Mg for the materials prepared at 550 °C suppresses the mixing of the Al2O3 interlayer with the film but forms MgyU1-yO2±x solid solutions during irradiation. Local thermal heating triggers the precipitation of a discontinuous crystalline MgO layer close to the film surface. The enhanced and selective diffusion of Mg into the film makes the materials prepared at 550 °C more robust and mechanically stable than those prepared at 350 °C.

Original languageEnglish
Pages (from-to)9850-9857
Number of pages8
JournalJournal of Physical Chemistry C
Volume127
Issue number20
DOIs
StatePublished - May 25 2023
Externally publishedYes

Funding

The work was performed with financial support in part from the US Department of Energy’s (DOE) National Nuclear Security Administration (NNSA, Grant # NA0004093) and the US National Science Foundation (NSF, PHY-2011890). KM also acknowledges funding from the US Army Research Office Grant # W911NF2110045 under the Materials Synthesis & Processing Program, with Dr. Michael P. Bakas as the program manager. The authors also acknowledge Notre Dame Integrated Imaging Facility (NDIIF) and Materials Characterization Facility (MCF) for instrumental usage.

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