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@ARTICLE{Ding:835983,
author = {Ding, R. and Rudakov, D. L. and Stangeby, P. C. and
Wampler, W. R. and Abrams, T. and Brezinsek, S. and
Briesemeister, A. and Bykov, I. and Chan, V. S. and Chrobak,
C. P. and Elder, J. D. and Guo, H. Y. and Guterl, J. and
Kirschner, A. and Lasnier, C. J. and Leonard, A. W. and
Makowski, M. A. and McLean, A. G. and Snyder, P. B. and
Thomas, D. M. and Tskhakaya, D. and Unterberg, E. A. and
Wang, H. Q. and Watkins, J. G.},
title = {{A}dvances in understanding of high- {Z} material erosion
and re-deposition in low- {Z} wall environment in
{DIII}-{D}},
journal = {Nuclear fusion},
volume = {57},
number = {5},
issn = {1741-4326},
address = {Vienna},
publisher = {IAEA},
reportid = {FZJ-2017-05108},
pages = {056016 -},
year = {2017},
abstract = {Dedicated DIII-D experiments coupled with modeling reveal
that the net erosion rate of high-Z materials, i.e. Mo and
W, is strongly affected by carbon concentration in the
plasma and the magnetic pre-sheath properties. Different
methods such as electrical biasing and local gas injection
have been investigated to control high-Z material erosion.
The net erosion rate of high-Z materials is significantly
reduced due to the high local re-deposition ratio. The ERO
modeling shows that the local re-deposition ratio is mainly
controlled by the electric field and plasma density within
the magnetic pre-sheath. The net erosion can be
significantly suppressed by reducing the sheath potential
drop. A high carbon impurity concentration in the background
plasma is also found to reduce the net erosion rate of
high-Z materials. Both DIII-D experiments and modeling show
that local 13CH4 injection can create a carbon coating on
the metal surface. The profile of 13C deposition provides
quantitative information on radial transport due to
E × B drift and the cross-field diffusion. The
deuterium gas injection upstream of the W sample can reduce
W net erosion rate by plasma perturbation. In H-mode
plasmas, the measured inter-ELM W erosion rates at different
radial locations are well reproduced by ERO modeling taking
into account charge-state-resolved carbon ion flux in the
background plasma calculated using the OEDGE code.},
cin = {IEK-4},
ddc = {530},
cid = {I:(DE-Juel1)IEK-4-20101013},
pnm = {174 - Plasma-Wall-Interaction (POF3-174)},
pid = {G:(DE-HGF)POF3-174},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000399125300003},
doi = {10.1088/1741-4326/aa6451},
url = {https://juser.fz-juelich.de/record/835983},
}