Abstract

The fusion excitation function of 48 Ti + 58 Fe has been measured in a wide energy range around the Coulomb barrier, covering 6 orders of magnitude of the cross sections. We present here the preliminary re- sults of this experiment, and a full comparison with the near-by system 58 Ni + 54 Fe where evidence of fusion hindrance shows up at relatively high cross sections. The sub-barrier cross sections of 48 Ti + 58 Fe are much larger than those of 58 Ni + 54 Fe. Significant differences are also observed in the logarithmic derivatives, astro- physical S-factors and fusion barrier distributions. The influence of low-energy nuclear structure on all these trends is pointed out and commented. Coupled-channels calculations using a Woods-Saxon potential are able to reproduce the experimental results for 48 Ti + 58 Fe. The logarithmic derivative of the excitation function is very nicely fit, and no evidence of hindrance is observed down to around 1 μb. The fusion barrier distribution is rather wide, flat and structureless. It is only in qualitative agreement with the calculated distribution.

Highlights

  • In the collision of two heavy ions at energies near and below the Coulomb barrier, couplings of the relative motion of the two nuclei to their low-energy surface vibrations and/or stable deformations [1, 2] determine the cross sections

  • The lower energy limit of such distributions, it has been shown in recent years [6, 7] that fusion excitation functions show a sharp decrease with decreasing energy, well below the expectations based on standard coupled-channels (CC) calculations

  • The fusion excitation function has been presented, and a significant irregularity of its logarithmic slope has been observed below the Coulomb barrier, but no evidence of hindrance shows up in the measured energy range

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Summary

Introduction

In the collision of two heavy ions at energies near and below the Coulomb barrier, couplings of the relative motion of the two nuclei to their low-energy surface vibrations and/or stable deformations [1, 2] determine the cross sections. Multi-phonon excitations have been shown [3] to become dominant for medium-heavy nuclei and produce complex fusion barrier distributions, possibly with discrete structures [4, 5]. The lower energy limit of such distributions, it has been shown in recent years [6, 7] that fusion excitation functions show a sharp decrease with decreasing energy, well below the expectations based on standard coupled-channels (CC) calculations.

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