Abstract

We present the first results of a comprehensive microscopic approach to describe nucleus-nucleus elastic collisions by means of an optical potential derived at first order in multiple-scattering theory and computed by folding the projectile and target nuclear densities with the nucleon-nucleon tt matrix, which describes the interaction between each nucleon of the projectile and each nucleon of the target. Chiral interactions are consistently used in the calculation of the tt matrix and of the nonlocal nuclear densities, which are computed within the ab initio no-core shell model. Cross sections calculated for αα collisions on 12^{12}C and 16^{16}O at projectile energies in the range 100-300 MeV are presented and compared with available data. For momentum transfer qq up to about 1.01.0 fm−1^{-1} our results are in good agreement with the experimental data, whereas for higher momenta a reduction of the imaginary contributions is needed.

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