Response of ZrC to swift heavy ion irradiation

Jacob Minnette, Evan Williams, William Cureton, Alexandre Solomon, Eric O’Quinn, Matthew Kurley, Rodney D. Hunt, Changyong Park, Ina Schubert, Christina Trautmann, Maik Lang

Research output: Contribution to journalArticlepeer-review

2 Scopus citations

Abstract

Zirconium carbide (ZrC) is commonly used for energy sector research, as well as a surrogate for the proposed advanced nuclear fuel candidate uranium carbide. This study investigates structural modifications to nanocrystalline and microcrystalline ZrC resulting from dense electronic excitations induced by swift heavy ion exposure. Samples were irradiated with 946 MeV Au ions to various fluences up to 6 × 1013 ions cm−2 and characterized using synchrotron-based x-ray diffraction. The evolution of the unit-cell parameter and heterogeneous microstrain were evaluated as a function of fluence and compared with those of nanocrystalline and microcrystalline CeO2 (a surrogate for UO2 fuel) irradiated under identical conditions. Distinct differences were observed in the radiation responses of the carbide and oxide across both grain sizes. Most notably, microcrystalline ZrC exhibits swelling characterized by two distinct regimes, which does not result in saturation at the ion fluences achieved. This contrasts with CeO2, which exhibits the well-documented direct-impact defect accumulation mechanism, reaching a steady-state saturation of swelling at higher fluences. Nanocrystalline CeO2 undergoes more pronounced swelling compared with microcrystalline CeO2, in contrast to nanocrystalline ZrC, which exhibits only minimal unit-cell changes. These results demonstrate that swift heavy ion-induced structural changes can be quite different in carbides and oxides, which must be considered when extrapolating fission-fragment type damage in current fuels to advanced fuels.

Original languageEnglish
Article number185901
JournalJournal of Applied Physics
Volume134
Issue number18
DOIs
StatePublished - Nov 14 2023

Funding

This work was funded by the Department of Energy (DOE) Office of Nuclear Energy's Nuclear Energy University Program under US-DOE, contract DE-NE0008895. J. Minnette acknowledges the support of the DOE/NNSA and the Chicago/DOE Alliance Center through cooperative agreement DE-NA0003975. A. Solomon acknowledges support from a Department of Energy, Office of Nuclear Energy University Nuclear Leadership Program Graduate Fellowship. Synchrotron XRD measurements were performed at HPCAT (Sector 16), Advanced Photon Source, Argonne National Laboratory. HPCAT operations are supported by DOE-NNSA's Office of Experimental Sciences. The Advanced Photon Source is a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. The results presented here are based on a UMAT experiment, which was performed at the M-branch beamline of the UNILAC at the GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt (Germany) in the frame of FAIR Phase-0. This manuscript has been authored by UT-Battelle, LLC, under contract DE-AC05-00OR22725 with the US Department of Energy (DOE). The US government retains and the publisher, by accepting the article for publication, acknowledges that the US government retains a nonexclusive, paid-up, irrevocable, worldwide license to publish or reproduce the published form of this manuscript, or allow others to do so, for US government purposes. DOE will provide public access to these results of federally sponsored research in accordance with the DOE Public Access Plan ( http://energy.gov/downloads/doe-public-access-plan ). This material is also based upon work supported under a Department of Energy, Office of Nuclear Energy University Nuclear Leadership Program Graduate Fellowship. This work was funded by the Department of Energy (DOE) Office of Nuclear Energy's Nuclear Energy University Program under US-DOE, contract DE-NE0008895. J. Minnette acknowledges the support of the DOE/NNSA and the Chicago/DOE Alliance Center through cooperative agreement DE-NA0003975. A. Solomon acknowledges support from a Department of Energy, Office of Nuclear Energy University Nuclear Leadership Program Graduate Fellowship. Synchrotron XRD measurements were performed at HPCAT (Sector 16), Advanced Photon Source, Argonne National Laboratory. HPCAT operations are supported by DOE-NNSA's Office of Experimental Sciences. The Advanced Photon Source is a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. The results presented here are based on a UMAT experiment, which was performed at the M-branch beamline of the UNILAC at the GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt (Germany) in the frame of FAIR Phase-0.

FundersFunder number
Advanced Photon Source
DOE-NNSA's Office of Experimental Sciences
Office of Nuclear Energy University
UNILAC
US-DOEDE-NE0008895
U.S. Department of Energy
Office of ScienceDE-AC02-06CH11357
Office of Nuclear Energy
National Nuclear Security AdministrationDE-NA0003975
Argonne National Laboratory
GSI Helmholtzzentrum für Schwerionenforschung

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