Lower hybrid current drive at high density in Alcator C-Mod
GM Wallace, AE Hubbard, PT Bonoli, IC Faust… - Nuclear …, 2011 - iopscience.iop.org
Nuclear Fusion, 2011•iopscience.iop.org
Experimental observations of lower hybrid current drive (LHCD) at high density on the
Alcator C-Mod tokamak are presented in this paper. Bremsstrahlung emission from
relativistic fast electrons in the core plasma drops suddenly above line-averaged densities of
10 20 m− 3 (ω/ω LH∼ 3) in single null discharges with large (⩾ 8 mm) inner gaps, well
below the density limit previously observed on limited tokamaks (ω/ω LH∼ 2). Modelling
and experimental evidence suggest that the absence of LHCD driven fast electrons at high …
Alcator C-Mod tokamak are presented in this paper. Bremsstrahlung emission from
relativistic fast electrons in the core plasma drops suddenly above line-averaged densities of
10 20 m− 3 (ω/ω LH∼ 3) in single null discharges with large (⩾ 8 mm) inner gaps, well
below the density limit previously observed on limited tokamaks (ω/ω LH∼ 2). Modelling
and experimental evidence suggest that the absence of LHCD driven fast electrons at high …
Abstract
Experimental observations of lower hybrid current drive (LHCD) at high density on the Alcator C-Mod tokamak are presented in this paper. Bremsstrahlung emission from relativistic fast electrons in the core plasma drops suddenly above line-averaged densities of 10 20 m− 3 (ω/ω LH∼ 3) in single null discharges with large (⩾ 8 mm) inner gaps, well below the density limit previously observed on limited tokamaks (ω/ω LH∼ 2). Modelling and experimental evidence suggest that the absence of LHCD driven fast electrons at high density may be due to parasitic collisional absorption in the scrape-off layer (SOL). Experiments show that the population of fast electrons produced by LHCD at high density () can be increased by operating with an inner gap of less than∼ 5 mm with the strongest non-thermal emission in inner wall limited plasmas. A change in plasma topology from single to double null produces a modest increase in non-thermal emission at high density. Increasing the electron temperature in the periphery of the plasma (0.8> r/a> 1.0) also results in a modest increase in non-thermal electron emission above the density limit. Ray tracing/Fokker–Planck simulations of these discharges predict the observed sensitivity to plasma position when the effects of collisional absorption in the SOL are included in the model.
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