Structure stability of (U, Pu) C and (U, Pu) N compositions

Atomic scale computer simulations based on density functional theory (DFT) are used to calculate the formation energies and structures associated with phases in the U-N, Pu-N, U-C and Pu-C systems. Stable phases across the compositional spaces, from the metal to the nitrogen gas or graphite end members, are identified using convex hull analysis. Many predicted phases correspond to those known from experimental phase diagrams (e.g. UN, U<sub>2</sub>N<sub>3</sub>; PuN; UC, U<sub>2</sub>C<sub>3</sub>; Pu<sub>2</sub>C<sub>3</sub>). However, many phases only sit on the convex hull upon inclusion of a suitably characterised Hubbard parameter (i.e. DFT + U). A nonstoichiometric composition of UN<sub>2-x</sub> is identified on the U-N convex hull but others, including stoichiometric UN<sub>2</sub>, are close to the line. A stoichiometric structure for Pu<sub>3</sub>C<sub>2</sub> with [Formula: see text] symmetry is identified, alongside which a nonstoichiometric PuC<sub>1-x</sub> phase has a similar energy.

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Publication Details

Journal
Scientific Reports
Published
2025-06-06
DOI
https://doi.org/10.1038/s41598-025-03910-y
Citations
3
Primary Topic
Nuclear Materials and Properties
Type
article
Field-Weighted Citation Impact
1.55

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article

Structure stability of (U, Pu) C and (U, Pu) N compositions

Robin W. Grimes, Sophie Cooper, Matthew K. Horton, William J. Watson
3 citations
Scientific Reports
Nuclear Materials and Properties
1.55
article

Structure stability of (U, Pu) C and (U, Pu) N compositions

Robin W. Grimes, Sophie Cooper, Matthew K. Horton, William J. Watson
article en
3 citations

Abstract

Atomic scale computer simulations based on density functional theory (DFT) are used to calculate the formation energies and structures associated with phases in the U-N, Pu-N, U-C and Pu-C systems. Stable phases across the compositional spaces, from the metal to the nitrogen gas or graphite end members, are identified using convex hull analysis. Many predicted phases correspond to those known from experimental phase diagrams (e.g. UN, U<sub>2</sub>N<sub>3</sub>; PuN; UC, U<sub>2</sub>C<sub>3</sub>; Pu<sub>2</sub>C<sub>3</sub>). However, many phases only sit on the convex hull upon inclusion of a suitably characterised Hubbard parameter (i.e. DFT + U). A nonstoichiometric composition of UN<sub>2-x</sub> is identified on the U-N convex hull but others, including stoichiometric UN<sub>2</sub>, are close to the line. A stoichiometric structure for Pu<sub>3</sub>C<sub>2</sub> with [Formula: see text] symmetry is identified, alongside which a nonstoichiometric PuC<sub>1-x</sub> phase has a similar energy.

Scientific ReportsVol. 15(1)
National Nuclear Laboratory (GB), Imperial College London (GB)
Imperial College London
Openalex Percentile: Top 18%
Nuclear Materials and Properties
1.55
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