Abstract
It is shown that a lower limit for the momentum transferred to the target nucleus by an incident fast charged particle may be obtained by measuring the directions of the emitted particles, without need to measure individual momenta. In cases with no unseen neutral particles, and negligible energy transfer, a value of the longitudinal momentum transfer may be obtained also. A technique is developed which is useful in distinguishing processes involving small momentum transfer, such as Coulomb and diffraction dissociation.
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