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Generation of high charge state platinum ions on vacuum arc plasma heated by gyrotron radiationa)
a)Contributed paper, published as part of the Proceedings of the 15th International Conference on Ion Sources, Chiba, Japan, September 2013.
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10.1063/1.4824644
/content/aip/journal/rsi/85/2/10.1063/1.4824644
http://aip.metastore.ingenta.com/content/aip/journal/rsi/85/2/10.1063/1.4824644
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Outline of gyrotron-driven test bench. 1—gyrotron, 2—input window with plasma gun, 3—magnetic trap, 4—plasma expander, 5—ion beam accelerating grid system, 6—vacuum chamber, 7—movable Faraday cup, and 8—time of flight spectrometer.

Image of FIG. 2.
FIG. 2.

Outline of ion source with cusp magnetic trap.

Image of FIG. 3.
FIG. 3.

Open magnetic trap with radial injection of vacuum arc plasma into the trap, based on four cathodes placed at the midplane of the trap (top) and the trap with axial injection of vacuum arc plasma into the trap from single plasma gun (bottom). Microwave input windows are located on the left side of traps.

Image of FIG. 4.
FIG. 4.

Ion charge state distributions (particle fractions) of extracted platinum ion beam without microwave heating (open columns) and with 37.5 GHz heating of vacuum arc plasma (closed columns) in cusp magnetic trap.

Image of FIG. 5.
FIG. 5.

Ion charge state distributions (particle fractions) of extracted platinum ion beam without microwave heating (open columns) and with 75 GHz heating of vacuum arc plasma (closed columns) in a mirror trap.

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/content/aip/journal/rsi/85/2/10.1063/1.4824644
2013-10-16
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Generation of high charge state platinum ions on vacuum arc plasma heated by gyrotron radiationa)
http://aip.metastore.ingenta.com/content/aip/journal/rsi/85/2/10.1063/1.4824644
10.1063/1.4824644
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