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Deuterium supersaturated surface layer in tungsten: ion energy dependence
by
Tynan, G. R.
, Patino, M. I.
, Schwarz-Selinger, T.
, Chang, F.
, Nishijima, D.
, Nagata, D.
, Simmonds, M. J.
, Založnik, A.
, Doerner, R. P.
, Tokitani, M.
, Baldwin, M. J.
2023
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Deuterium supersaturated surface layer in tungsten: ion energy dependence
by
Tynan, G. R.
, Patino, M. I.
, Schwarz-Selinger, T.
, Chang, F.
, Nishijima, D.
, Nagata, D.
, Simmonds, M. J.
, Založnik, A.
, Doerner, R. P.
, Tokitani, M.
, Baldwin, M. J.
2023
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Deuterium supersaturated surface layer in tungsten: ion energy dependence
Journal Article
Deuterium supersaturated surface layer in tungsten: ion energy dependence
2023
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Abstract
Properties of deuterium (D) supersaturated surface layers (DSSLs) formed in tungsten (W), such as thickness, internal microstructures, and D retention, are experimentally investigated as a function of the incident ion energy, E i . W samples were exposed to D plasmas in the PISCES-A linear plasma device in a range of E i ∼ 45–175 eV, while other plasma exposure parameters were fixed: sample temperature, T s , ∼423 K, ion flux, Γ i , ∼1.2 × 10 21 m −2 s −1 , and fluence, Φ i , ∼3.0 × 10 24 m −2 . High-resolution, cross-sectional, transmission electron microscopy observations confirm that (1) a DSSL forms even at the lowest E i ∼ 45 eV, (2) the DSSL thickness, Δ t DSSL , is found to decrease with decreasing E i from ∼11–12 nm at E i ∼ 175 eV to ∼5–6 nm at ∼45 eV, and to agree with approximately the maximum implantation depth calculated using SDTrimSP, and (3) high-density D nanobubbles with a diameter of ∼1 nm or less exist inside the DSSL, which is deemed to validate a theory-predicted vacancy stabilization process due to trapping of a solute D atom(s). Utilizing a D areal density of ∼4.2 × 10 19 m −2 in the first 14 nm from the surface at E i ∼ 75 eV from nuclear reaction analysis and the measured E i dependence of Δ t DSSL , our previous laser-induced breakdown spectroscopy data is updated: both dynamic and static D retention increase with decreasing E i , and the D/W atomic fraction during plasma exposure reaches ∼0.3 at E i ∼ 45 eV. A possible DSSL formation mechanism is proposed.
Publisher
IOP Publishing
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