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@ARTICLE{Hakola:904048,
author = {Hakola, A. and Likonen, J. and Lahtinen, A. and Vuoriheimo,
T. and Groth, M. and Kumpulainen, H. and Balden, M. and
Krieger, K. and Mayer, M. and Schwarz-Selinger, T. and
Brezinsek, S. and Kelemen, M. and Markelj, S. and Barac, M.
and Gouasmia, S. and Bogdanovic Radovic, I. and Uccello, A.
and Vassallo, E. and Dellasega, D. and Passoni, M. and Sala,
M. and Bernard, E. and Diez, M. and Guillemaut, C. and
Tsitrone, E. and Team, the ASDEX Upgrade and Team, the
EUROfusion MST1 and Contributors, the EUROfusion WP PFC},
title = {{G}ross and net erosion balance of plasma-facing materials
in full-{W} tokamaks},
journal = {Nuclear fusion},
volume = {61},
number = {11},
issn = {0029-5515},
address = {Vienna},
publisher = {IAEA},
reportid = {FZJ-2021-05618},
pages = {116006 -},
year = {2021},
abstract = {Gross and net erosion of tungsten (W) and other
plasma-facing materials in the divertor region have been
investigated in deuterium (D) and helium (He) plasmas during
dedicated experiments in L- and H-mode on ASDEX Upgrade and
after full-length experimental campaigns on the WEST
tokamak. Net erosion was determined via post-exposure
analyses of plasma-exposed samples and full-size wall
components, and we conclude that the same approach is
applicable to gross erosion if marker structures with
sub-millimeter dimensions are used to eliminate the
contribution of prompt re-deposition. In H-mode plasmas,
gross erosion during ELMs may exceed the situation in
inter-ELM conditions by 1–2 orders of magnitude while net
erosion is typically higher by a factor of 2–3. The
largest impact on net erosion is attributed to the electron
temperature while the role of the impurity mixtures is
weaker, even though both on ASDEX Upgrade and WEST
significant amounts of impurities are present in the edge
plasmas. Impurities, on the other hand, will lead to the
formation of thick co-deposited layers. We have also noted
that with increasing surface roughness, net erosion is
strongly suppressed and the growth of co-deposited layers is
enhanced. In He plasmas, gross erosion is increased compared
to D due to the higher mass and charge states of the plasma
particles, resulting from larger energies due to sheath
acceleration, but strong impurity fluxes can result in
apparent net deposition in the divertor. Our results from
ASDEX Upgrade and WEST are comparable and indicate typical
net-erosion rates of 0.1–0.4 nm s−1, excluding the
immediate vicinity of the strike-point regions.},
cin = {IEK-4},
ddc = {620},
cid = {I:(DE-Juel1)IEK-4-20101013},
pnm = {134 - Plasma-Wand-Wechselwirkung (POF4-134)},
pid = {G:(DE-HGF)POF4-134},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000704879400001},
doi = {10.1088/1741-4326/ac22d2},
url = {https://juser.fz-juelich.de/record/904048},
}