Impact of minority concentration on fundamental (H)D ICRF heating performance in JET-ILW

ITER will start its operation with non-activated hydrogen and helium plasmas at a reduced magnetic field of B0 = 2.65 T. In hydrogen plasmas, the two ion cyclotron resonance frequency (ICRF) heating schemes available for central plasma heating (fundamental H majority and 2nd harmonic 3He minority ICRF heating) are likely to suffer from relatively low RF wave absorption, as suggested by numerical modelling and confirmed by previous JET experiments conducted in conditions similar to those expected in ITER's initial phase. With 4He plasmas, the commonly adopted fundamental H minority heating scheme will be used and its performance is expected to be much better. However, one important question that remains to be answered is whether increased levels of hydrogen (due to e.g. H pellet injection) jeopardize the high performance usually observed with this heating scheme, in particular in a full-metal environment. Recent JET experiments performed with the ITER-like wall shed some light onto this question and the main results concerning ICRF heating performance in L-mode discharges are summarized here.

[1]  J. Contributors,et al.  Spectroscopic investigation of heavy impurity behaviour during ICRH with the JET ITER-like wall , 2014 .

[2]  J. Contributors,et al.  Effect of the minority concentration on ion cyclotron resonance heating in presence of the ITER-like wall in JET , 2014 .

[3]  Lorenzo Figini,et al.  ICRF-code benchmark activity in the framework of the European Task-Force on Integrated Tokamak Modelling , 2014 .

[4]  C. Giroud,et al.  On the challenge of plasma heating with the JET metallic wall , 2013, 1309.0948.

[5]  E. Joffrin,et al.  Comparison of long term fuel retention in JET between carbon and the ITER-Like Wall , 2013 .

[6]  R. Neu,et al.  ICRF specific plasma wall interactions in JET with the ITER-like wall , 2013 .

[7]  J. Contributors,et al.  Characterisation of local ICRF heat loads on the JET ILW , 2013, 1306.6778.

[8]  J. Byun,et al.  Atmospheric-pressure plasma sources for biomedical applications , 2012 .

[9]  J. Contributors,et al.  Impurity production from the ion cyclotron resonance heating antennas in JET , 2012 .

[10]  R. Felton,et al.  Experimental investigation of ion cyclotron range of frequencies heating scenarios for ITER's half-field hydrogen phase performed in JET , 2012 .

[11]  D. McCune,et al.  Benchmarking ICRF full-wave solvers for ITER , 2012 .

[12]  D. V. Eester,et al.  A 1D model for describing ion cyclotron resonance heating at arbitrary cyclotron harmonics in tokamak plasmas , 2013 .

[13]  C. Giroud,et al.  ICRF scenarios for ITER's half-field phase , 2011 .

[14]  M. N. A. Beurskens,et al.  JET ITER-like wall—overview and experimental programme , 2011 .

[15]  R. Felton,et al.  Optimizing ion-cyclotron resonance frequency heating for ITER: dedicated JET experiments , 2011 .

[16]  E. Lerche,et al.  Simple 1D Fokker–Planck modelling of ion cyclotron resonance frequency heating at arbitrary cyclotron harmonics accounting for Coulomb relaxation on non-Maxwellian populations , 2011 .

[17]  J. Contributors,et al.  Metal impurity transport control in JET H-mode plasmas with central ion cyclotron radiofrequency power injection , 2011 .

[18]  Jet Efda Contributors,et al.  Experimental verification of sawtooth control by energetic particles in ion cyclotron resonance heated JET tokamak plasmas , 2010 .

[19]  Daniele Milanesio,et al.  Performance of the ITER ICRH system as expected from TOPICA and ANTITER II modelling , 2010 .

[20]  L. Giannone,et al.  Assessment of compatibility of ICRF antenna operation with full W wall in ASDEX Upgrade , 2010 .

[21]  J. Contributors,et al.  Modelling of D majority ICRH at JET: impact of absorption at the Doppler-shifted resonance , 2009 .

[22]  J. Cordey,et al.  Physics of high power ICRH on Jet , 2008 .

[23]  F. W. Baity,et al.  ICRF Heating Experiments on DIII‐D , 2008 .

[24]  Jet Efda Contributors,et al.  Improved break-in-slope analysis of the plasma energy response in tokamaks , 2008 .

[25]  G. T. Hoang,et al.  On the role of ion heating in ICRF heated discharges in Tore Supra , 2001 .

[26]  R. König,et al.  Analysis of bulk ion heating with ICRH in JET high-performance plasmas , 1999 .

[27]  D. V. Eester,et al.  A variational principle for studying fast-wave mode conversion , 1998 .

[28]  A. Gondhalekar,et al.  Impurity induced neutralization of megaelectronvolt energy protons in JET plasmas , 1997 .

[29]  J. Rice,et al.  Survey of ICRF heating experiments and enhanced performance modes in Alcator C-Mod , 1996 .

[30]  F. Durodié,et al.  Ion Cyclotron Resonance Heating on TEXTOR , 2005 .

[31]  Charles F. F. Karney Fokker-Planck and Quasilinear Codes , 1986, physics/0501066.

[32]  T. H. Stix Fast-wave heating of a two-component plasma , 1975 .