The high-power helicon program at DIII-D: gearing up for first experiments

• Published in: Nuclear fusion Vol. 61; no. 11; pp. 116034 - 116046
• Main Authors: Van Compernolle, B., Brookman, M.W., Moeller, C.P., Pinsker, R.I., Garofalo, A.M., O’Neill, R., Geng, D., Nagy, A., Squire, J.P., Schultz, K., Pawley, C., Ponce, D., Torrezan, A.C., Lohr, J., Coriton, B., Hinson, E., Kalling, R., Marinoni, A., Martin, E.H., Nguyen, R., Petty, C.C., Porkolab, M., Raines, T., Ren, J., Rost, C., Schmitz, O., Torreblanca, H., Wang, H.Q., Watkins, J., Zeller, K.
• Format: Journal Article
• Language: English
• Published: United States IOP Publishing 01.11.2021; IOP Science
• Subjects: 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; current drive; fast wave; helicon; reactor relevant
• ISSN: 0029-5515; 1741-4326; 1741-4326
• DOI: 10.1088/1741-4326/ac25c0

Helicon current drive, also called fast wave current drive in the lower hybrid range of frequencies, has long been regarded as a promising current drive tool for reactor grade plasmas. A newly installed MW-level system at DIII-D will be the first test of this technology in reactor-relevant plasmas, in the sense that full single-pass absorption is expected. A 30-module traveling wave antenna has been installed and optimized in-vessel in early 2020. The linear electromagnetic characteristics of the unloaded module array have been extensively tested both on the bench and in the vessel at instrumentation power levels. Excellent performance has been achieved, ~2% reflected power and ~1.5% dissipated power per module in air, in a 10 MHz band around 476 MHz. Stripline feeds on both ends of the antenna allow either co or counter current drive. The installation of a 1.2 MW klystron and associated high-power electronics was completed in Fall 2020. Commissioning of the antenna is ongoing. An important goal of this experiment is to validate the helicon current drive physics basis using an extensive set of new and upgraded diagnostics.