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We present recent SANS results concerning the modelling of helium bubble growth in F82H-mod.
Knowledge of radiation-induced helium bubble nucleation and growth in SiC is essential for applications in fusion and fission environments.
Hydrogen may be trapped by He-V clusters, or He clusters or very small helium bubble seed to help bubble nucleation [17].
While the helium bubble size distribution becomes narrower with increasing dose, the average size of bubbles remains unchanged and the density of bubbles increases somewhat with dose.
These investigations may provide new insight into the underlying mechanisms of helium bubble nucleation and formation in the Zr/Ti2AlC interface.
The helium bubble density was found to increase with ion energy in pillars, roughly from 8.2% to 48.4%, and to increase with increasing PPI, from 36.4% to 116.2%, and with bubble concentrations up to 9.1 × 1021 m−3.
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The nucleation and growth of helium (He) bubbles in the bulk and at Σ3〈1 1 0〉{1 1 2} and Σ73b〈1 1 0〉{6 6 1} grain boundaries (GBs) in bcc iron have been investigated using molecular dynamics simulations.
Argon, a gas, was flushed out by a stream of helium bubbles and then trapped in ultracold charcoal.
Most hydrogen atoms were trapped by helium bubbles.
But bubbles in this study are supposed to be helium bubbles with some hydrogen.
Kong et al. [7] studied the influence of Au ion irradiation damage on helium-implanted tungsten, used Orowan stress formula [8] to interpret the interaction between helium bubbles and irradiation defects in tungsten materials and found helium bubbles as impenetrable obstacles for the dislocation motion, and thought the density and size of helium bubbles were the key factors for hardening.
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