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Generation of Supersonic and Super-Alfvénic Flow Using ICRF Heating and a Magnetic Nozzle

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Figure

Fig. 1Schematic of the HITOP device.
Fig. 3Dependence of ΔW⊥ on the downstream magnetic fieldBD. He plasma. The solid and dashed lines correspond toω/ωci = 1 and 2, respectively, for the wave frequenciesof fRF = 237 kHz.
Fig. 8Axial profile of (a) magnetic field and (b) ion Mach num-ber Mi and Alfv´en Mach number MA in the divergingmagnetic nozzle configurations.

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