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N. Castin, M. Chiapetto, C. Domain, C. Becquart

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1 N. Castin, M. Chiapetto, C. Domain, C. Becquart
OKMC model for FeNiMn with solute transport: first results and importance of method of analysis N. Castin, M. Chiapetto, C. Domain, C. Becquart and L. Malerba

2 Synopsis What did we do? How was the solute transport modelled?
We introduced explicit solute transport in an object kinetic Monte Carlo model We applied it to study an FeMnNi alloy How was the solute transport modelled? Ni and Mn dragged by single point-defects, as according to the latest DFT studies What did we obtain? Spontaneous formation of solute clusters around point-defect clusters. Analyse the results with the eyes of APT Comparison with experimental measurement shows encouraging signs

3 Grey alloy OKMC approach : solute clusters are associated with point-defect clusters
SIA clusters Number density of Mn-Ni precipitates according to APT is of the order of the density of TEM-invisible SIA clusters  Assumed to be solute clusters! Atomistic simulations reveal that loops make Mn-Ni ppts stable NUMBER DENSITY (m-3) TEM-visible SIA clusters (>90 SIA, 1.3 nm) G. Bonny et al., Journal of Nuclear Materials 452 (2014) 486 How to introduce solute transport in an OKMC model where solutes are not present?

4 Key atomistic mechanism: solute dragging by point defects
In general, one may expect that a solute atom will move via vacancy in the opposite direction to the vacancy A V Instead, Mn and Ni, but also Cu, Si, and P, follow the vacancy during its migration B Fe V Fe Mn / P Fe Finally, any solute forming a mixed dumbbell wil be dragged by it Fe

5 DFT-based models reveal that all solutes found in clusters in RPV steels are dragged by point defects VACANCY DRAG INTERSTITIAL TRANSPORT Vacancy can carry solute atoms along. Occurring for manganese, nickel, copper, phosphorus, silicon. Interstital atoms can couple with solute atoms and move together. Occurring for manganese, phosphorus, chromium. Flux-coupling phenomena Formation of pecipitates and solute segregation in RPV steels Low T diffusion coefficinets L. Messina, P. Olsson, M. Nastar, T. Garnier, C. Domain, PRB 90, (2014) L. Messina, IGRDM-18

6 Atomistic KMC provides DFT-based parameters to describe Ni & Mn transport when dragged by point-defects The fastest and most stable diffuser is the Mn via dumbbell Single-vacancies drag both Mn & Ni Mn slightly more efficiently dragged because of lower migration energy Small point-defect clusters will also contribute to solute transport but this is neglected in first approximation

7 New MATEO software developed @ SCK•CEN
Hybrid A/OKMC model New MATEO software SCK•CEN OKMC for microstructure, AKMC for solute transport Only single point-defects transport solutes Solute transport by mobile clusters is disregarded Each time a point-defect finds a solute, a new object (solute-Va pair, mixed dumbbell, …) is created The binding energy defines for how long the point-defect drags the solute, i.e. until dissociation Correlation effects with surrounding solutes are disregarded C atoms are simulated as traps and most parameters are the same as in the grey alloys model Alternative: remove traps and consider that the defect falls randomly in a “trapped status” Here the slide is unchanged compared to last conference. Message is slightly changed: 1°) The hybrid OKMC – AKMC model is inherently going to predict lots of clusters of solute atoms, around nearly all fixed trap. Presented like this, it looks like the model fails because the density of solute clusters is 1 or 1.5 orders of magnitude too high compared to APT measurements. 2°) There are improvable aspects of the model from a physical point of view, as will be shown in the next slides 2.1 – Fixed traps could be avoided by introducing explicit C, even though this is far easier to say than to do. 2.2 – More mechanisms of solute transport, so far neglected for simplicity, could be added with the desired effect to dilute some clusters 3°) Last but not least, the results of our simulation are not 1-to-1 comparable to APT. This is important because some solute clusters might be invisible by APT. REMARK: I hope the circles supposed to represent SIA’s will remain grey on your computer, because otherwise it becomes confusing. They appeared white on my computer, i.e. identical to vacancies.

8 Problem: excess of clusters produced around Va-traps
Possible reasons Overestimation of solute transport – unlikely because of DFT based parameter and neglect of clusters … No mechanism for solute-vacancy cluster dissolution NEW: analysis does not take into account APT features! New MATEO software SCK•CEN

9 Introduction of mechanisms of dissolution
Mechanism of dissolution introduced as limiting case: all emitted vacancies carry a solute out Solute-vacancy complex Solutes - Vac Solute + Vac Solute + SIA Surviving Vac cluster Accumulating solutes Releasing few of them. Annihilated Vac cluster leaving solutes behind New MATEO software SCK•CEN

10 Introduction of mechanisms of dissolution
Dissolution of SIA-solute complexes forbidden because of high thermal stability Solute-SIA complex Solute - SIA Solute + Vac Solute + SIA Surviving SIA cluster Accumulating solutes Releasing none of them. Annihilated SIA cluster with solutes left behind New MATEO software SCK•CEN

11 Model improved but still no good agreement

12 Looking at our result from the simulation with the eyes of the APT
Emulating the effects of APT measurements Apply detection probability Apply random perturbations of atomic coordinates Search for clusters using defendable algorithm in alignment with what APT people do. Most impacting effect The smallest clusters are “dissolved”, i.e. not anymore identifiable as cluster. XY-plane Large perturbation ! (up to 1nm) 40% of atoms detected in while sample Z-axis Small perturbation

13 Our results after the APT treatment
Results are in excellent agreement with experiment! Our overall model for the formation of solute clusters is consistent with experimental evidence, provided that the analysis is performed with the “eyes” of the experimental technique!

14 Summary & Outlook Dragging of solutes by point-defects leading to segregation of solutes on point-defect clusters has been identified as the key mechanism leading to formation of solute clusters in iron alloys and specifically RPV steels A hybrid Object/Atomistic KMC model (new code Mateo) has been developed to include explicitly the transport of solutes Its use with a "not-too-unrealistic“ set of parameters leads to the formation of solute clusters in the correct amount and of the correct size Outlook: verify the model in all its parts (visible loops, …) and develop the parameterisation further, to have a single all-including model L. Messina, IGRDM-18 15


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