The NSC KIPT sited charged particles accelerators are widely used to support R&D of radiation damage physics and radiation material science. The accelerator based "simulation" irradiation of materials is supplementing the standard practice of their large-scale reactor tests and is an economically efficient resource saving technique of the express assessment of their behavior and performance in a totally controllable irradiation environment.
Beryllium, one of the most studied functional material of nuclear engineering, manifests the non-trivial properties and effects (e.g., superplasticity) promoted by its pronounced anisotropy. This also applies to the impact of point defects on its electronic structure and the low-temperature transport properties particularly regarding the structural sensitivity of its superconducting transition temperature Tc.
In 2017 SPE RESST R&D, the previously developed methodology and software for multiscale computer modeling of radiation effects have been applied to the characterization and planning of cryogenic irradiations of beryllium at the NSC KIPT electron linac ELIAS. By the successive application of the methods of microscopic atomistic, mesoscopic kinetic and macroscopic continuum modeling, the influence of the anisotropy of Be lattice on the accumulation of radiation damage under electron irradiation at various temperatures is elucidated along with the influence, on it, of the initial dislocation structure of irradiated targets.
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Figure 1 – The Frenkel pairs (FP) production rate depth profiles of Be primary radiation damage by electrons of different energies. Monte Carlo (MC) calculations in the NRT standard approximation (O) and by the SPE RESST MC code RaT explicit modeling of atomic collisions cascades (♦)
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Figure 2 – The Sandia SPPARKS code kinetic Monte Carlo simulation of Be SIA (♦) diffusion, recombination with vacancies (♦), and trapping by differently directed edge dislocation sinks. T = 77 K
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Figure 3 – The atomic concentrations of residual vacancies plotted vs. those of the primary Frenkel pairs (FPpa) initially produced at an electron beam exposure time t0 (top axis) in Be targets of various dislocation densities ρd (solid curves) in comparison with those predicted with a simplified isotropic model (dashed curves).
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