The dependence of confinement on the isotope mass in the core and the edge of AUG and JET-ILW H-mode plasmas
Author(s) -
P. A. Schneider,
C. Angioni,
L. Frassinetti,
L. Horváth,
M. Maslov,
F. Auriemma,
M. Cavedon,
C. Challis,
E. Delabie,
M. Dunne,
J.M. Fontdecaba,
J. Hobirk,
A. Kappatou,
D. Keeling,
B. Kurzan,
M. Lennholm,
B. Lomanowski,
C. F. Maggi,
R. M. McDermott,
T. Pütterich,
A. Thorman,
M. Willensdorfer,
the ASDEX Upgrade Team,
the EUROfusion MST Team,
Jet Contributors
Publication year - 2021
Publication title -
nuclear fusion
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.774
H-Index - 120
eISSN - 1741-4326
pISSN - 0029-5515
DOI - 10.1088/1741-4326/ac3e82
Subject(s) - pedestal , asdex upgrade , plasma , jet (fluid) , core (optical fiber) , ion , atomic physics , physics , isotope , tokamak , materials science , scaling , nuclear physics , mechanics , optics , geometry , archaeology , quantum mechanics , mathematics , history
Experiments in ASDEX Upgrade (AUG) and JET with the ITER-like wall (JET-ILW) are performed to separate the pedestal and core contributions to confinement in H-modes with different main ion masses. A strong isotope mass dependence in the pedestal is found which is enhanced at high gas puffing. This is because the ELM type changes when going from D to H for matched engineering parameters, which is likely due to differences in the inter ELM transport with isotope mass. The pedestal can be matched in H and D plasmas by varying only the triangularity and keeping the engineering parameters relevant for core transport the same. With matched pedestals Astra/TGLF (Sat1geo) core transport simulations predict the experimental profiles equally well for H and D. These core transport simulations show a negligible mass dependence and no gyro-Bohm scaling is observed. However, to match the experimental observations at medium β it is required to take the fast-ion dilution and rotation into account. This is not enough for high β plasmas where for the first time a profile match between H and D plasmas was achieved experimentally. Under these conditions quasilinear modelling with TGLF over predicts the transport in the core of H and D plasmas alike.
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