Global Viewpoint on Nuclear-Particle-Emission Cross Sections at Intermediate Energies
M. Iwasaki
Abstract
M. Iwasaki
Abstract
It follows from the independent-particle picture of the nucleus that the cross section for the reaction ($d$, $^{6}\mathrm{Li}$) depends upon the target mass number $A$ as $\ensuremath{\sim}{A}^{\ensuremath{-}3.33}$, indicating the significance of a recent empirical observation. The energy-integrated cross sections for emission of $p$, $d$, $^{3}\mathrm{H}$, $^{3}\mathrm{He}$, and $^{4}\mathrm{He}$ from Mg, Ni, and Ag nuclei bombarded by a 235-MeV pion beam show some features suggestive of nuclear structure.
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It follows from the independent-particle picture of the nucleus that the cross section for the reaction ($d$, $^{6}\mathrm{Li}$) depends upon the target mass number $A$ as $\ensuremath{\sim}{A}^{\ensuremath{-}3.33}$, indicating the significance of a recent empirical observation. The energy-integrated cross sections for emission of $p$, $d$, $^{3}\mathrm{H}$, $^{3}\mathrm{He}$, and $^{4}\mathrm{He}$ from Mg, Ni, and Ag nuclei bombarded by a 235-MeV pion beam show some features suggestive of nuclear structure.
Key concepts: Physics, Atomic physics, Cross section (physics), Nuclear reaction, Nuclear physics, Pion, Particle (ecology), Energy (signal processing)