Characterization and performance of a field aligned ion cyclotron range of frequency antenna in Alcator C-Moda)

Ion cyclotron range of frequency (ICRF) heating is expected to provide auxiliary heating for ITER and future fusion reactors where high Z metallic plasma facing components (PFCs) are being considered. Impurity contamination linked to ICRF antenna operation remains a major challenge particularly for devices with high Z metallic PFCs. Here, we report on an experimental investigation to test whether a field aligned (FA) antenna can reduce impurity contamination and impurity sources. We compare the modification of the scrape of layer (SOL) plasma potential of the FA antenna to a conventional, toroidally aligned (TA) antenna, in order to explore the underlying physics governing impurity contamination linked to ICRF heating. The FA antenna is a 4-strap ICRF antenna where the current straps and antenna enclosure sides are perpendicular to the total magnetic field while the Faraday screen rods are parallel to the total magnetic field. In principle, alignment with respect to the total magnetic field minimizes integrated E|| (electric field along a magnetic field line) via symmetry. A finite element method RF antenna model coupled to a cold plasma model verifies that the integrated E|| should be reduced for all antenna phases. Monopole phasing in particular is expected to have the lowest integrated E||. Consistent with expectations, we observed that the impurity contamination and impurity source at the FA antenna are reduced compared to the TA antenna. In both L and H-mode discharges, the radiated power is 20%–30% lower for a FA-antenna heated discharge than a discharge heated with the TA-antennas. However, inconsistent with expectations, we observe RF induced plasma potentials (via gas-puff imaging and emissive probes to be nearly identical for FA and TA antennas when operated in dipole phasing). Moreover, the highest levels of RF-induced plasma potentials are observed using monopole phasing with the FA antenna. Thus, while impurity contamination and sources are indeed reduced with the FA antenna configuration, the mechanism determining the SOL plasma potential in the presence of ICRF and its impact on impurity contamination and sources remains to be understood.

[1]  J. Terry,et al.  Ion-cyclotron range of frequencies in the scrape-off-layer: fine structure radial electric fields , 2012 .

[2]  S. Wukitch,et al.  Mitigation of radio frequency sheaths through magnetic field-aligned ICRF antenna design , 2012 .

[3]  X. Litaudon,et al.  Characterization of heat flux generated by ICRH heating with cantilevered bars and a slotted box Faraday screen , 2012 .

[4]  J L Terry,et al.  Vacuum ultraviolet impurity spectroscopy on the Alcator C-Mod tokamak. , 2010, The Review of scientific instruments.

[5]  L. Colas,et al.  Reduction of RF-sheaths potentials by compensation or suppression of parallel RF currents on ICRF antennas , 2009 .

[6]  I. Hutchinson,et al.  Two dimensional radiated power diagnostics on Alcator C-Mod. , 2006, The Review of scientific instruments.

[7]  B. Lipschultz,et al.  Influence of boronization on operation with high-Z plasma facing components in Alcator C-Mod , 2007 .

[8]  H. Greuner,et al.  Final Steps to an All Tungsten Divertor Tokamak , 2007 .

[9]  S. J. Wukitch,et al.  Diagnostic Systems on Alcator C-Mod , 2007 .

[10]  B. Lipschultz Operation of Alcator C-Mod with high-Z plasma facing components and implications , 2005 .

[11]  V. Basiuk,et al.  Theory and Practice in ICRF Antennas for Long Pulse Operation , 2005 .

[12]  D. Russell,et al.  Nonlinear ICRF-plasma interactions , 2005 .

[13]  David R. Smith,et al.  A study of molybdenum influxes and transport in Alcator C-Mod , 2001 .

[14]  Current Drive Chapter 6: Plasma auxiliary heating and current drive , 1999 .

[15]  F. G. Rimini,et al.  D-T fusion with ion cyclotron resonance heating in the JET tokamak , 1998 .

[16]  J. Rice,et al.  H mode confinement in Alcator C-Mod , 1997 .

[17]  P. M. Ryan,et al.  ICRF/Edge Interaction Guidelines for ICRF Antenna Design and Initial ICRF/Edge Interaction Experiments on the Tore Supra Tokamak , 1996 .

[18]  Murakami,et al.  Ion cyclotron range of frequency heating of a deuterium-tritium plasma via the second-harmonic tritium cyclotron resonance. , 1995, Physical review letters.

[19]  D. A. D’Ippolito,et al.  Far field sheaths from waves in the ion cyclotron range of frequencies , 1994 .

[20]  P. T. Bonoli,et al.  First results from Alcator‐C‐MOD* , 1994 .

[21]  J. Jacquinot,et al.  Radio‐frequency‐sheath‐driven edge plasma convection and interaction with the H mode , 1993 .

[22]  J. Jacquinot,et al.  Effect of beryllium evaporation on the performance of ICRH on JET , 1990 .

[23]  F. W. Perkins,et al.  Radiofrequency sheaths and impurity generation by ICRF antennas , 1989 .

[24]  Richard Majeski,et al.  Secondary electron emission‐capacitive probes for plasma potential measurements in plasmas with hot electrons , 1987 .

[25]  H. Verbeek,et al.  Data Compendium for Plasma-Surface Interactions , 1984 .

[26]  J. Bohdansky,et al.  An analytical formula and important parameters for low‐energy ion sputtering , 1980 .