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One could make a distinction between a classical trajectory study such as this one, in which a single ellipse was taken to represent the initial state, and one in which all classical orbital parameters, major-axis directions, etc., are appropriately distributed in intervals to correspond to quantum-mechanical states. The latter approach is referred to generally as the classical-trajectory Monte Carlo (CTMC) approach, but the terms CT and CTMC will be used interchangeably here. In our CT calculations for the 24 top state only the dynamically indeterminate initial position of the electron in its Keplerian orbit and the impact-parameter vectors of incident ions were averaged. The full CTMC approach is represented, e.g., by
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