2017
DOI: 10.1016/j.jnucmat.2017.09.002
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Quantitative evaluation of hydrogen atoms trapped at single vacancies in tungsten using positron annihilation lifetime measurements: Experiments and theoretical calculations

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Cited by 15 publications
(21 citation statements)
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“…The decrease in τ 2 after hydrogen charging is 21 ps and 26 ps (on average 23.5 ps) at doses of 1.4 × 10 −4 dpa and 2.9 × 10 −4 dpa, respectively. The simulations show that the PAL decreases by approximately 15 ps and 10 ps when the first and second hydrogen atoms are added to the vacancies, respectively [7]. It is expected that one or two hydrogen atoms (on average 1.8 atoms) are captured by one vacancy in this study, which is similar to that seen in a previous study (on average 1.6 atoms, 5.8 MPa pressure) [7].…”
Section: Methodssupporting
confidence: 86%
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“…The decrease in τ 2 after hydrogen charging is 21 ps and 26 ps (on average 23.5 ps) at doses of 1.4 × 10 −4 dpa and 2.9 × 10 −4 dpa, respectively. The simulations show that the PAL decreases by approximately 15 ps and 10 ps when the first and second hydrogen atoms are added to the vacancies, respectively [7]. It is expected that one or two hydrogen atoms (on average 1.8 atoms) are captured by one vacancy in this study, which is similar to that seen in a previous study (on average 1.6 atoms, 5.8 MPa pressure) [7].…”
Section: Methodssupporting
confidence: 86%
“…The de-trapping rate is defined as the product of the concentration of the vacant interstitial hydrogen sites, hydrogen jump frequency for de-trapping, and concentration of hydrogen trapped at the vacancies. Based on [7] and Sieverts' law, we set the maximum number of hydrogen atoms (Z) that the vacancies can capture at 6, while the binding energy of hydrogen to the vacancies and hydrogen concentration were 1.19 eV and 4.6 × 10 −12 (Pressure: 1 MPa, Temperature: 573 K), respectively. Furthermore, the jump frequencies for trapping and de-trapping were assumed to be equal.…”
Section: Resultsmentioning
confidence: 99%
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