I. B. Khriplovich, D. A. Solovyev
Published 2016-03-19Version 1
We consider the electromagnetic production of positron in collision of heavy nuclei, with the simultaneously produced electron captured by one of the nuclei. This cross-section exceeds by about four orders of magnitude the cross-section of $e^+ e^-$ production.
Comments: 3 pages, 1 figure
$π^+ - π^-$ Asymmetry and the Neutron Skin in Heavy Nuclei
Proxy-SU(3) symmetry in heavy nuclei: Foundations
Theory of the electromagnetic production of hyperons
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