A standard fourth-order Runge Kutta method is used for numerical integration of the ion trajectory in three dimensions.
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This occurs because the repulsive potential of the target atom bends close ion trajectories away from their original path, and is referred to as " blocking ".
3.
Eventually, the unmagnetized, massive ions are fast enough that the weak electric and magnetic forces in the downstream region become insufficient to deflect the ion trajectories except for extremely high magnetic strengths.
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