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Using AORSA to simulate helicon waves in DIII-D

Recent efforts have shown that helicon waves (fast waves at > 20ωci) may be an attractive option for driving efficient off-axis current drive during non-inductive tokamak operation for DIII-D, ITER and DEMO. For DIII-D scenarios, the ray tracing code, GENRAY, has been extensively used to study he...

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Main Authors: Lau, Cornwall, Jaeger, E. F., Bertelli, Nicola, Berry, Lee Alan, Blazevski, Daniel, Green, David, Murakami, Masanori, Park, J. M., Pinsker, R. I., Prater, R.
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container_volume 1689
creator Lau, Cornwall
Jaeger, E. F.
Bertelli, Nicola
Berry, Lee Alan
Blazevski, Daniel
Green, David
Murakami, Masanori
Park, J. M.
Pinsker, R. I.
Prater, R.
description Recent efforts have shown that helicon waves (fast waves at > 20ωci) may be an attractive option for driving efficient off-axis current drive during non-inductive tokamak operation for DIII-D, ITER and DEMO. For DIII-D scenarios, the ray tracing code, GENRAY, has been extensively used to study helicon current drive efficiency and location as a function of many plasma parameters. The full wave code, AORSA, which is applicable to arbitrary Larmor radius and can resolve arbitrary ion cyclotron harmonic order, has been recently used to validate the ray tracing technique at these high cyclotron harmonics. If the SOL is ignored, it will be shown that the GENRAY and AORSA calculated current drive profiles are comparable for the envisioned high beta advanced scenarios for DIII-D, where there is high single pass absorption due to electron Landau damping and minimal ion damping. AORSA is also been used to estimate possible SOL effects on helicon current drive coupling and SOL absorption due to collisional and slow wave effects.
doi_str_mv 10.1063/1.4936534
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source American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list)
subjects Absorption
Cyclotrons
Ions
Landau damping
Larmor radius
Nuclear power plants
Plasma
Ray tracing
Tokamak devices
title Using AORSA to simulate helicon waves in DIII-D
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