16O contamination in 4He analysis beams
The 4He + beam from a Van de Graaff accelerator is often accompanied by an 16O + beam of the same energy. If, after acceleration and before magnetic analysis, one electron is stripped from the oxygen ion to form 16O 2+, these ions will not be separated from 4He + during magnetic analysis. The 16O 2+...
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Veröffentlicht in: | Thin solid films 1973-12, Vol.19 (2), p.371-380 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The
4He
+ beam from a Van de Graaff accelerator is often accompanied by an
16O
+ beam of the same energy. If, after acceleration and before magnetic analysis, one electron is stripped from the oxygen ion to form
16O
2+, these ions will not be separated from
4He
+ during magnetic analysis. The
16O
2+ fraction in the
4He
+ beam was measured by analyzing back-scattering spectra for a thin Au film and the O to He ion charge ratio of 2:1 was confirmed by electrostatic deflection. Ion source conditions and the pressure in the beam lines strongly affect the
16O
2+ fraction and the dependence of the O
2+/O
+ ratio on pressure is found to be in approximate agreement with predicted values. A formula for estimating the
16O
2+ beam intensity, based on charge exchange data and measurement of the primary
16O
+ beam intensity, is
N[
O
2+] = 13
P(
torr)
l(
cm)
N[
O
+], where
P is the total gas pressure,
l the length of the beam line between the accelerator and switching magnet and
N[O
2+] and
N[O
+] are the beam intensities of the respective species. The
16O
2+ contamination of
4He
+ beams is easily removed by electrostatic separation. |
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ISSN: | 0040-6090 1879-2731 |
DOI: | 10.1016/0040-6090(73)90073-4 |