2016
DOI: 10.1103/physrevb.94.024103
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Ab initioscaling laws for the formation energy of nanosized interstitial defect clusters in iron, tungsten, and vanadium

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Cited by 96 publications
(124 citation statements)
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References 62 publications
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“…For tungsten, the majority of existing potentials struggle to reproduce the correct trend of the relative stability of clusters of multiple SIAs. For example, several widely used EAM potentials predict dislocation loops with the Burgers vector 1 0 0 to be lower in energy than the 1/2 1 1 1 loops [5], which is in clear contradiction to DFT [82] and experimental observations [83,84]. We therefore put particular focus on ensuring that our GAP reproduces the expected trend obtained by DFT.…”
Section: Self-interstitial Atoms and Clustersmentioning
confidence: 90%
See 1 more Smart Citation
“…For tungsten, the majority of existing potentials struggle to reproduce the correct trend of the relative stability of clusters of multiple SIAs. For example, several widely used EAM potentials predict dislocation loops with the Burgers vector 1 0 0 to be lower in energy than the 1/2 1 1 1 loops [5], which is in clear contradiction to DFT [82] and experimental observations [83,84]. We therefore put particular focus on ensuring that our GAP reproduces the expected trend obtained by DFT.…”
Section: Self-interstitial Atoms and Clustersmentioning
confidence: 90%
“…13 shows formation energies of parallel 1 1 1 and 1 0 0 SIA clusters (i.e. dislocation loops) compared between the GAP and DFT data from [82]. 1/2 1 1 1 clusters are created by inserting parallel dumbbells with a (1 1 0) habit plane, and 1 0 0 with a (1 0 0) plane, as in [82].…”
Section: Self-interstitial Atoms and Clustersmentioning
confidence: 99%
“…2.37 ± 0.06 7.39 ± 0.20 4.92 ± 0.29 1.22 ± 0.01 0.39 ± 0.03 0.87 ± 0.04 Table 7: Linear regression fits for the formation energy (in eV) and relaxation volume Ω rel /Ω 0 of interstitial clusters in the C15 structure. Energies are fitted to E f = a 0 N +a 1 N 2/3 +a 2 , as suggested by ref [52], indicating terms dependent on volume and surface area. Relaxation volume are fitted to Ω rel /Ω 0 = b 0 N + b 1 N 2/3 + b 2 .…”
Section: The Anisotropy Of the Elastic Relaxationmentioning
confidence: 99%
“…Relaxation volume are fitted to Ω rel /Ω 0 = b 0 N + b 1 N 2/3 + b 2 . The structures taken were those used in ref [52], using the cell relaxation method, with sizes 2 ≤ N ≤ 22. 4).…”
Section: The Anisotropy Of the Elastic Relaxationmentioning
confidence: 99%
“…The bottom figure shows similar histograms for cluster sizes 2-13 interstitials. Inset: a comparison of the binding energy for the minimum energy structures computed with DFT[74]…”
mentioning
confidence: 99%