As the extraction hole is 1.5 cm in radius and the emitter electrode is 5.0 cm in radius, around 25 mA should be extracted.
As the plasma does not penetrate close to the gap, the focusing fields are very strong and the beam is quickly brought to a waist. The lack of any transverse space-charge force allows the beam particles to cross-over. As the beam is very small in the defocusing field region of the gap it sees little force and emerges as a highly divergent beam.
This case shows the lowest aberrations (phase-space diagram below the animation) strongly suggesting that space-charge is the major force for aberrations in the other higher density cases.
back to home... | prepared by Richard Scrivens | 23rd January 1998 |