1980
DOI: 10.1016/0022-3115(80)90302-5
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Important sputtering yield data for tokamaks: A comparison of measurements and estimates

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Cited by 59 publications
(16 citation statements)
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“…This would tend to be too high a value for elements lighter than Al. 46 We shall not work with Eqns (20) and (21) any further but simply note that this simple approach is useful but less precise than the approaches of Matsunami et al 3 and Yamamura and Tawara. 4 In the fits of the data 7,8,24 -26 for 28 elements as listed above, the difference between the curves for Matsunami Figure 2.…”
Section: Fitting To Published Experimental Datamentioning
confidence: 96%
See 1 more Smart Citation
“…This would tend to be too high a value for elements lighter than Al. 46 We shall not work with Eqns (20) and (21) any further but simply note that this simple approach is useful but less precise than the approaches of Matsunami et al 3 and Yamamura and Tawara. 4 In the fits of the data 7,8,24 -26 for 28 elements as listed above, the difference between the curves for Matsunami Figure 2.…”
Section: Fitting To Published Experimental Datamentioning
confidence: 96%
“…Because the fitting of the data depends on the function used for S n E and the data selected, there is inevitably some variation between˛Ł and E th that may be anti-correlated. Bohdansky 19,20 expresses the threshold effects with rather more complex terms than in Eqn. (8) but focuses on the energy regime below 600 eV to study the effects of light ion sputtering in the tokamak where the plasma strikes the containment wall.…”
mentioning
confidence: 99%
“…For a given projectile and target, there exists a minimum projectile kinetic energy needed to induce sputtering. This energy is called the threshold energy (E th ), and is given by (Bohdansky et al, 1980;Anderson & Bay, 1981)…”
Section: Sputteringmentioning
confidence: 99%
“…For a given projectile and target, there exists a minimum projectile kinetic energy needed to induce sputtering. This energy is called the threshold energy (E th ), and is given by (Bohdansky et al, 1980;Anderson & Bay, 1981) )where M 1 is the projectile mass, M 2 is the mean molecular mass per atom of the target, and β, the maximum fractional energy transfer possible in a head-on elastic collision, is given by 2 2 1 2 1 ) (…”
Section: Sputteringmentioning
confidence: 99%
“…(1972), Coburn et al . (1977) (1971), Bohdansky (1980), Oliva-Florio et al . (1987) and Fitch & Mahmound (1982).…”
Section: )mentioning
confidence: 99%