Hauptseite > Publikationsdatenbank > Laser-Induced Desorption of co-deposited Deuterium in Beryllium Layers on Tungsten > print |
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100 | 1 | _ | |a Zlobinski, M. |0 P:(DE-Juel1)172037 |b 0 |e Corresponding author |
245 | _ | _ | |a Laser-Induced Desorption of co-deposited Deuterium in Beryllium Layers on Tungsten |
260 | _ | _ | |a Amsterdam [u.a.] |c 2019 |b Elsevier |
336 | 7 | _ | |a article |2 DRIVER |
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520 | _ | _ | |a For the development of the tritium monitoring system in ITER the hydrogen isotope release by Laser-Induced Desorption (LID) from Be layers is studied to determine the laser parameters for a high desorption efficiency while minimising dust production and surface modifications is also pursued. Be layers of 1 µm thickness with 25–30 at% D and 3 × 1022 D/m2 comparable to JET-ILW areal concentrations [1] have been produced by High Power Impulse Magnetron Sputtering (HiPIMS) on ITER grade W. Laser pulses of 1, 5 and 10 ms duration heat the layer in vacuum in the Fuel REtention DIagnostic Setup (FREDIS) and release the retained D thermally. By mass spectrometry in FREDIS and subsequent Nuclear Reaction Analysis (NRA) inside the laser spot the desorbed and remaining D is quantified. While a pulse duration of 1 ms cannot fully desorb the deuterium, it is found that a single 5 or 10 ms laser pulse with an absorbed energy density of ca. 1.5 MJ/m2 corresponding to a heat flux factor around 20 MW√s/m2 leads to nearly complete desorption of the retained D. This encourages the development of a useful tritium monitoring system, although the present layers produce some dust due to local delamination of the layer on at least 11% of the heated surface (at 1.4 MJ/m2 absorbed energy within 5 ms) and lead to unavoidable crack formation. |
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773 | _ | _ | |a 10.1016/j.nme.2019.04.007 |g Vol. 19, p. 503 - 509 |0 PERI:(DE-600)2808888-8 |p 503 - 509 |t Nuclear materials and energy |v 19 |y 2019 |x 2352-1791 |
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