Far infrared laser polarimeter development for the C-2 field reversed configuration plasmas
November 2013 | B. Deng | APS-DPP | Poster
Ideal FRC configuration has zero toroidal field.
November 2013 | B. Deng | APS-DPP | Poster
Ideal FRC configuration has zero toroidal field.
November 2013 | F. Cecherini | APS-DPP | Poster
The generation and propagation of an ion cyclotron resonant wave is studied in a Field Reversed Configuration (FRC) plasma which includes at least two different ion species.
November 2013 | S. Aefsky | APS-DPP | Poster
The electron temperature of the plasma inside the C-2 Experiment is measured using a Thomson Scattering (TS) diagnostic.
November 2013 | R. Magee | APS-DPP | Poster
The C-2 field-reversed configuration (FRC) plasmas are created via the dynamic merging of two compact toroids and partially sustained through the injection of high power neutral beams.
November 2013 | K. Zhai | APS-DPP | Poster
C2 Thomson scattering system is upgraded with capability of electron density profile measurement.