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Effects of projectile track charging on the H− secondary ion velocity distribution

The bombardment of insulating targets by MeV projectiles produces a positive track delivering secondary electrons to the solid. These electrons are eventually captured by adsorbed hydrogen-containing molecules, inducing fragmentation and initiating the H− secondary ion emission. The dynamics of this...

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Bibliographic Details
Published in:Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms Beam interactions with materials and atoms, 2007-03, Vol.256 (1), p.483-488
Main Authors: Iza, P., Farenzena, L.S., da Silveira, E.F.
Format: Article
Language:English
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Summary:The bombardment of insulating targets by MeV projectiles produces a positive track delivering secondary electrons to the solid. These electrons are eventually captured by adsorbed hydrogen-containing molecules, inducing fragmentation and initiating the H− secondary ion emission. The dynamics of this process is very sensitive to the track electric field and depends on the emission site and on the H− initial velocity. In this work, a model, based on a time-depending track potential followed by secondary electron induced desorption – SEID, is employed to describe the production and dynamics of H− secondary ion emission. It is shown that depending on how fast the track neutralization occurs, the movement of H− ions may be accelerated, decelerated or even aborted. Trajectories, angular distributions and energy distributions are predicted and compared with experimental data obtained for water ice bombarded by 1.7MeV nitrogen ions.
ISSN:0168-583X
1872-9584
DOI:10.1016/j.nimb.2006.12.070