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@ARTICLE{Reinke:837458,
author = {Reinke, M. L. and Meigs, A. and Delabie, E. and Mumgaard,
R. and Reimold, F. and Potzel, S. and Bernert, M. and
Brunner, D. and Canik, J. and Cavedon, M. and Coffey, I. and
Edlund, E. and Harrison, J. and LaBombard, B. and Lawson, K.
and Lomanowski, B. and Lore, J. and Stamp, M. and Terry, J.
and Viezzer, E.},
title = {{E}xpanding the role of impurity spectroscopy for
investigating the physics of high-{Z} dissipative divertors},
journal = {Nuclear materials and energy},
volume = {12},
issn = {2352-1791},
address = {Amsterdam [u.a.]},
publisher = {Elsevier},
reportid = {FZJ-2017-06371},
pages = {91-99},
year = {2017},
abstract = {New techniques that attempt to more fully exploit
spectroscopic diagnostics in the divertor and pedestal
region during highly dissipative scenarios are demonstrated
using experimental results from recent low-Z seeding
experiments on Alcator C-Mod, JET and ASDEX Upgrade. To
exhaust power at high parallel heat flux, q∥ > 1 GW/m2,
while minimizing erosion, reactors with solid, high-Z plasma
facing components (PFCs) are expected to use extrinsic
impurity seeding. Due to transport and atomic physics
processes which impact impurity ionization balance,
so-called ‘non-coronal’ effects, we do not accurately
know and have yet to demonstrate the maximum q∥ which can
be mitigated in a tokamak. Radiation enhancement for
nitrogen is shown to arise primarily from changes in Li- and
Be-like charge states on open field lines, but also through
transport-driven enhancement of H- and He-like charge states
in the pedestal region. Measurements are presented from
nitrogen seeded H-mode and L-mode plasmas where emission
from N through N are observed. Active charge exchange
spectroscopy of partially ionized low-Z impurities in the
plasma edge is explored to measure N and N within the
confined plasma, while passive UV and visible spectroscopy
is used to measure N-N in the boundary. Examples from recent
JET and Alcator C-Mod experiments which employ nitrogen
seeding highlight how improving spectroscopic coverage can
be used to gain empirical insight and provide more data to
validate boundary simulations.},
cin = {IEK-4},
ddc = {333.7},
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:000417293300012},
doi = {10.1016/j.nme.2016.12.003},
url = {https://juser.fz-juelich.de/record/837458},
}