P. Napolitani

High-resolution velocity measurements on fully identified light nuclides produced in Fe-56 + hydrogen and Fe-56 + titanium systems

New experimental results on the kinematics and the residue production are obtained for the interactions of

Measurement of the complete nuclide production and kinetic energies of the system {sup 136}Xe+hydrogen at 1 GeV per nucleon

^{56}\mathrm{Fe}

Spallation residues in the reaction Fe-56 + p at 0.3-A-GeV, 0.5, 0.75, 1.0-A GeV and 1.5 A GeV

projectiles with protons and

Evidence for α-particle condensation in nuclei from the Hoyle state deexcitation

^{\mathrm{nat}}\mathrm{Ti}

Production of medium-mass neutron-rich nuclei in reactions induced by Xe 136 projectiles at 1 A GeV on a beryllium target

target nuclei, respectively, at the incident energy of

In-medium effects for nuclear matter in the Fermi-energy domain

1\phantom{\rule{0.3em}{0ex}}A\phantom{\rule{0.3em}{0ex}}\mathrm{GeV}

Understanding transport simulations of heavy-ion collisions at 100A and 400A MeV: Comparison of heavy-ion transport codes under controlled conditions

. The titanium-induced reaction serves as a reference case for multifragmentation. Already in the proton-induced reaction, the characteristics of the isotopic cross sections and the shapes of the velocity spectra of light residues indicate that high thermal energy is deposited in the system during the collision. In the

Bifurcations in Boltzmann–Langevin one body dynamics for fermionic systems

^{56}\mathrm{Fe}+p

New isospin effects in central heavy-ion collisions at Fermi energies

system the high excitation seems to favor the onset of fast break-up decays dominated by very asymmetric partitions of the disassembling system. This configuration leads to the simultaneous formation of one or more light fragments together with one heavy residue.

Inclusive selection of intermediate-mass-fragment formation modes in the spallation of 136Xe

We present an extensive overview of production cross sections and kinetic energies for the complete set of nuclides formed in the spallation of {sup 136}Xe by protons at the incident energy of 1 GeV per nucleon. The measurement was performed in inverse kinematics at the GSI fragment separator. Slightly below the Businaro-Gallone point, {sup 136}Xe is the stable nuclide with the largest neutron excess. The kinematic data and cross sections collected in this work for the full nuclide production are a general benchmark for modeling the spallation process in a neutron-rich nuclear system, where fission is characterized by predominantly mass-asymmetric splits.