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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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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 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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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. |
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ISSN: | 0168-583X 1872-9584 |
DOI: | 10.1016/j.nimb.2006.12.070 |