The total elastic nucleon–nucleus cross-section is calculated at energies up to 600 MeV for the elements [Formula: see text]C, [Formula: see text]Pb, [Formula: see text]O, 9Be, 4He, 2H, [Formula: see text]U and [Formula: see text]Al using a finite electromagnetic potential, which is obtained considering a Randall–Sundrum II scenario modified by the inclusion of [Formula: see text] compact extra dimensions. The length scale bound is set in the potential to compare with known experimental data.
The elastic differential cross section is calculated at low energies (below 100 MeV) for the elements 3He, 20Ne, 40Ar, 14N, 12C, and for the 208Pb using a finite electromagnetic potential, which is obtained by considering a Randall–Sundrum II scenario modified by the inclusion of p compact extra-dimensions. The length scale is adjusted in the potential to compare with known experimental data and to set bounds for the parameter of the model. The effective four-dimensional (4D) electromagnetic potential is produced by a point charge, as seen from the three-brane that contains it, in uniform motion in an RSIIp scenario.
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