Abstract
The interplay between atomic and nuclear interactions in heavy ion collisions with nuclear contact is studied. The general theoretical description is outlined and analyzed in a number of different limits (semiclassical approximation, DWBA, fully quantal description). The two most important physical mechanisms for generating atomic-nuclear interference, i.e., energy conservation and the introduction of additional phase shifts by nuclear reactions, are extracted. The resulting typical coupling matrix elements are analyzed for their relative importance in atomic and nuclear excitations. The description of nuclear influence on atomic excitations in terms of a classical time delay caused by nuclear reactions is reviewed, and its relationship to the underlying quantal character of the nuclear reaction is discussed.
The theory is applied to spontaneous positron emission in supercritical heavy-ion collisions (Ztot ≥173). It is shown that nuclear contact can lead to line structures in the positron energy spectra if the probability distribution for nuclear delay times caused by the contact has contributions for T ≥ 10-19 sec. We explicitly evaluate a model where a pocket in the internuclear potential near the touching configuration leads to formation of nuclear molecules, and predict a resonance-like excitation function for the positron peak.
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© 1987 Plenum Press, New York
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Heinz, U. (1987). Quantum Mechanical Theory of Positron Production in Heavy Ion Collisions with Nuclear Contact. In: Greiner, W. (eds) Physics of Strong Fields. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-1889-7_23
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DOI: https://doi.org/10.1007/978-1-4613-1889-7_23
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