Abstract
A semiempirical model describing the direct breakup of light nuclei by low-energy nucleons is proposed. The model is based upon the assumption that a statistical equilibrium is established with respect to the incident particle and (ν1) tightly bound subgroup components of the target nucleus inside of an energy-dependent interaction volume. The interaction volume is taken to be an oblate spheroid which is oriented along the direction of the incident particle path, and which has a minor axis equal to the de Broglie wavelength λ, and a major axis equal to (R+aλ), where R and a are parameters characteristic to the particular reaction involved. The direct breakup cross section is calculated for the Be9(n, 2n)Be8 and C12(n, n)3He4 reactions.

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