October 2019 | D. Kobayashi | APS-DPP | Poster
The technique for injection an impurity ion-doped CT has been proposed. The TCCT is produced and accelerated by an MCPG with a tracer source injector.
October 2019 | J.B. Titus | APS-DPP | Poster
In TAE Technologies’ current experimental device, C-2W (also called “Norman”),1 record breaking, advanced beam-driven field reversed configuration (FRC)
October 2019 | Marcel Nations | APS-DPP | Poster
The diagnostic provides spatially- and temporally- resolved measurements of key impurity ion parameters. Impurity ion velocity (Doppler shift).
October 2019 | E.M. Granstedt | APS-DPP | Poster
NB model accounts for grid size, divergence, duct loss Primary edge neutral source: plasma and neutral wall recycling. Bump in neutral density at 0.2 m
October 2019 | Timothy DeHaas | APS-DPP | Poster
In TAE Technologies’ current experimental device, C2W (also called “Norman”) [1], record breaking, advanced beam-driven field reversed configuration (FRC) plasmas are produced and sustained in steady state utilizing variable energy neutral beams,
October 2019 | Roger J Smith | APS-DPP | Poster
In TAE Technologies’ current experimental device, C-2W (also called “Norman”) [1], record breaking, advanced beam- driven field reversed configuration (FRC)