TY - JOUR
T1 - Pedestal and e r profile evolution during an edge localized mode cycle at ASDEX Upgrade
AU - Asdex Upgrade Team, The
AU - Cavedon, M.
AU - Pütterich, T.
AU - Viezzer, E.
AU - Laggner, F. M.
AU - Burckhart, A.
AU - Dunne, M.
AU - Fischer, R.
AU - Lebschy, A.
AU - Mink, F.
AU - Stroth, U.
AU - Willensdorfer, M.
AU - Wolfrum, E.
N1 - Publisher Copyright:
© 2017 IOP Publishing Ltd.
PY - 2017/8/17
Y1 - 2017/8/17
N2 - The upgrade of the edge charge exchange recombination spectroscopy diagnostic at ASDEX Upgrade has enabled highly spatially resolved measurements of the impurity ion dynamics during an edge-localized mode cycle (ELM) with unprecedented temporal resolution, i.e. 65 μs. The increase of transport during an ELM induces a relaxation of the ion, electron edge gradients in impurity density and flows. Detailed characterization of the recovery of the edge temperature gradients reveals a difference in the ion and electron channel: the maximum ion temperature gradient is re-established on similar timescales as , which is faster than the recovery of . After the clamping of the maximum gradient, T i and T e at the pedestal top continue to rise up to the next ELM while n e stays constant which means that the temperature pedestal and the resulting pedestal pressure widen until the next ELM. The edge radial electric field E r at the ELM crash is found to reduce to typical L-mode values and its maximum recovers to its pre-ELM conditions on a similar time scale as for n e and T i. Within the uncertainties, the measurements of E r align with their neoclassical predictions for most of the ELM cycle, thus indicating that E r is dominated by collisional processes. However, between 2 and 4 ms after the ELM crash, other contributions to flow, e.g. zonal flows or ion orbit effects, could not be excluded within the uncertainties.
AB - The upgrade of the edge charge exchange recombination spectroscopy diagnostic at ASDEX Upgrade has enabled highly spatially resolved measurements of the impurity ion dynamics during an edge-localized mode cycle (ELM) with unprecedented temporal resolution, i.e. 65 μs. The increase of transport during an ELM induces a relaxation of the ion, electron edge gradients in impurity density and flows. Detailed characterization of the recovery of the edge temperature gradients reveals a difference in the ion and electron channel: the maximum ion temperature gradient is re-established on similar timescales as , which is faster than the recovery of . After the clamping of the maximum gradient, T i and T e at the pedestal top continue to rise up to the next ELM while n e stays constant which means that the temperature pedestal and the resulting pedestal pressure widen until the next ELM. The edge radial electric field E r at the ELM crash is found to reduce to typical L-mode values and its maximum recovers to its pre-ELM conditions on a similar time scale as for n e and T i. Within the uncertainties, the measurements of E r align with their neoclassical predictions for most of the ELM cycle, thus indicating that E r is dominated by collisional processes. However, between 2 and 4 ms after the ELM crash, other contributions to flow, e.g. zonal flows or ion orbit effects, could not be excluded within the uncertainties.
KW - edge gradient recovery
KW - edge localized mode
KW - ion temperature
KW - radial electric field
UR - http://www.scopus.com/inward/record.url?scp=85029939259&partnerID=8YFLogxK
U2 - 10.1088/1361-6587/aa7ad0
DO - 10.1088/1361-6587/aa7ad0
M3 - Article
AN - SCOPUS:85029939259
SN - 0741-3335
VL - 59
JO - Plasma Physics and Controlled Fusion
JF - Plasma Physics and Controlled Fusion
IS - 10
M1 - 105007
ER -