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 t 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 t matrix and of the nonlocal nuclear densities, which are computed within the ab initio no-core shell model. Cross sections calculated for α collisions on ^{12}C and ^{16}O at projectile energies in the range 100-300 MeV are presented and compared with available data. For momentum transfer q up to about 1.0 fm^{-1} our results are in good agreement with the experimental data, whereas for higher momenta a reduction of the imaginary contributions is needed.
Vorabbi, M., Gennari, M., Finelli, P., Giusti, C., Navrátil, P. (2025). Toward a Microscopic Description of Nucleus-Nucleus Collisions. PHYSICAL REVIEW LETTERS, 135(17), 1-6 [10.1103/qxtf-5b4y].
Toward a Microscopic Description of Nucleus-Nucleus Collisions
Finelli, Paolo
;
2025
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 t 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 t matrix and of the nonlocal nuclear densities, which are computed within the ab initio no-core shell model. Cross sections calculated for α collisions on ^{12}C and ^{16}O at projectile energies in the range 100-300 MeV are presented and compared with available data. For momentum transfer q up to about 1.0 fm^{-1} our results are in good agreement with the experimental data, whereas for higher momenta a reduction of the imaginary contributions is needed.| File | Dimensione | Formato | |
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