% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Zlobinski:864234,
author = {Zlobinski, M. and Sergienko, G. and Martynova, Y. and
Matveev, D. and Unterberg, B. and Brezinsek, S. and Spilker,
B. and Nicolai, D. and Rasinski, M. and Möller, S. and
Linsmeier, Ch. and Lungu, C. P. and Porosnicu, C. and Dinca,
P. and De Temmerman, G.},
title = {{L}aser-{I}nduced {D}esorption of co-deposited {D}euterium
in {B}eryllium {L}ayers on {T}ungsten},
journal = {Nuclear materials and energy},
volume = {19},
issn = {2352-1791},
address = {Amsterdam [u.a.]},
publisher = {Elsevier},
reportid = {FZJ-2019-04068},
pages = {503 - 509},
year = {2019},
abstract = {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.},
cin = {IEK-4 / IEK-1 / IEK-2},
ddc = {624},
cid = {I:(DE-Juel1)IEK-4-20101013 / I:(DE-Juel1)IEK-1-20101013 /
I:(DE-Juel1)IEK-2-20101013},
pnm = {174 - Plasma-Wall-Interaction (POF3-174)},
pid = {G:(DE-HGF)POF3-174},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000470746100079},
doi = {10.1016/j.nme.2019.04.007},
url = {https://juser.fz-juelich.de/record/864234},
}