TY - JOUR
T1 - The improved H-mode at ASDEX Upgrade
T2 - A candidate for an ITER hybrid scenario
AU - Staebler, A.
AU - Sips, A. C.C.
AU - Brambilla, M.
AU - Bilato, R.
AU - Dux, R.
AU - Gruber, O.
AU - Hobirk, J.
AU - Horton, L. D.
AU - Maggi, C. F.
AU - Manini, A.
AU - Maraschek, M.
AU - Mück, A.
AU - Na, Y. S.
AU - Neu, R.
AU - Tardini, G.
AU - Wade, M. R.
PY - 2005/7/1
Y1 - 2005/7/1
N2 - A stationary regime with improved confinement (H98(y, 2) > 1) and, simultaneously, improved stability (βN > 2.5) compared to standard H-mode has been investigated on ASDEX Upgrade for many years. This so-called 'improved H-mode' is characterized by a q-profile with low central magnetic shear and q0 ≥ 1 that is obtained by early heating during the current ramp. Studies of this discharge scenario have been continued. New results are presented concerning the existence domain in the q95 range, the dependence on the normalized Larmor radius and initial experiments showing that high performance improved H-modes can be obtained with strong central ion cyclotron resonance heating (ICRH). In addition, the present status of understanding of the improved H-mode is reviewed. Improved H-mode plasmas are documented for 3.2 < q95 < 4.5 and ne/n GW up to 0.85. At low densities the normalized collisionality ν* is close to the ITER value and within the range of , accessible in ASDEX Upgrade, no dependence of the performance on this parameter was found. When compared with standard H-mode, core transport is still governed by drift-wave turbulence. Impurity control is achieved by central wave heating. The improved stability is due to the q-profile: by q0 > 1 sawteeth as the main trigger of large amplitude neoclassical tearing modes are avoided. The stability is eventually limited by the occurrence of a mode with poloidal mode number m ≤ 2 and toroidal mode number n ≤ 1 at typically βN ∼ 3. As far as the reactor relevance of this regime is concerned, its compatibility with significant central electron heating by ICRH, with high edge densities and low amplitude edge localized modes is of importance. The improved H-mode is, therefore, seen as a candidate for a long pulse ITER 'hybrid' operation.
AB - A stationary regime with improved confinement (H98(y, 2) > 1) and, simultaneously, improved stability (βN > 2.5) compared to standard H-mode has been investigated on ASDEX Upgrade for many years. This so-called 'improved H-mode' is characterized by a q-profile with low central magnetic shear and q0 ≥ 1 that is obtained by early heating during the current ramp. Studies of this discharge scenario have been continued. New results are presented concerning the existence domain in the q95 range, the dependence on the normalized Larmor radius and initial experiments showing that high performance improved H-modes can be obtained with strong central ion cyclotron resonance heating (ICRH). In addition, the present status of understanding of the improved H-mode is reviewed. Improved H-mode plasmas are documented for 3.2 < q95 < 4.5 and ne/n GW up to 0.85. At low densities the normalized collisionality ν* is close to the ITER value and within the range of , accessible in ASDEX Upgrade, no dependence of the performance on this parameter was found. When compared with standard H-mode, core transport is still governed by drift-wave turbulence. Impurity control is achieved by central wave heating. The improved stability is due to the q-profile: by q0 > 1 sawteeth as the main trigger of large amplitude neoclassical tearing modes are avoided. The stability is eventually limited by the occurrence of a mode with poloidal mode number m ≤ 2 and toroidal mode number n ≤ 1 at typically βN ∼ 3. As far as the reactor relevance of this regime is concerned, its compatibility with significant central electron heating by ICRH, with high edge densities and low amplitude edge localized modes is of importance. The improved H-mode is, therefore, seen as a candidate for a long pulse ITER 'hybrid' operation.
UR - http://www.scopus.com/inward/record.url?scp=15944392372&partnerID=8YFLogxK
U2 - 10.1088/0029-5515/45/7/009
DO - 10.1088/0029-5515/45/7/009
M3 - Article
AN - SCOPUS:15944392372
SN - 0029-5515
VL - 45
SP - 617
EP - 625
JO - Nuclear Fusion
JF - Nuclear Fusion
IS - 7
ER -