April 2013 | F. Cecherini | Sherwood Fusion Theory | Presentation
The Field Reversed Configuration (FRC) exhibits very peculiar structures for both the plasma density and the magnetic field.
April 2013 | M. Onofri | Sherwood Fusion Theory | Presentation
A 2D transport code (Q2D) is used to study the evolution of C2 Field Reversed Configuration with neutral beam injection.
February 2013 | H. Gota | Nihon Symposium | Presentation
Demonstration of a High Performance FRC (HPF) operating regime by combining effects of edge-biasing from an end-plasma-gun and of neutral-beam injection.
February 2013 | M. Tuszewski | Nihon Symposium | Presentation
FRCs permit to use advanced fusion fuels.
February 2013 | L. Steinhauer | Nihon Symposium | Presentation
Five critical near-term issues.
February 2013 | H. Guo | EPR Workshop | Presentation
FRC offers an ideal configuration for an economic reactor and may allow use of aneutronic fuels.
January 2013 | S. Dettrick | 2013 Energetic Particles Workshop UCI | Presentation
Without magnetic perturbations, NB Ion energy confinement time is τE~ 500us. Most NB ion energy goes to heating electrons.
November 2012 | D. Barnes | APS-DPP | Presentation
November 2012 | B. Deng | APS-DPP | Poster
Bolometer data show that the plasma spin is in the ion diamagnetic direction, while the plasma column wobbles in the electron diamagnetic direction.
November 2012 | E. Garate | APS-DPP | Poster
We are implementing additional scintillator based neutron detectors on the TAE Technologies C-2 system.