Abstract

The angular dependence of the electronic energy loss of fast ions was calculated. Models for the transitions from axial to planar channeling and from planar channeling to a random direction are discussed in terms of a simple generalization of the Lindhard–Jin–Gibson Model for the axial–random transition. In order to compare these models with experimental data, the energy loss of 2.0 MeV He ions channeled through a thin silicon crystal into directions that scan the {0 0 1} plane from the [1 1 0] axis to the [1 0 0] axis was measured.

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