As the extraction hole is 1.5 cm in radius and the emitter electrode is 5.0 cm in radius, around 130 mA should be extracted.
The extracted ion beam is then pricipally focused by the gap fields (not the plasma meniscus) and then the transverse space-charge and the defocusing field of the second half of the gap produce reduce the beams angles, but without causing a space-charge explosion.
The resulting beam has a low total divergence and is therefore the closest to the matched case for this extraction geometry and voltages.
Below the animation is shown the resulting phase-space. Even though these conidtions give the lowest divergence we can see a large amount of aberration in the resulting emittance. This aberration is the spherical aberration of the electrostatic lens, but this may then couple into the beam due to the space-charge field to further disrupt the beam.
back to home... | prepared by Richard Scrivens | 23rd January 1998 |