Analysis of the nuclear potential for heavy-ion systems through large-angle quasi-elastic scattering
The knowledge of the nuclear potential between two colliding nuclei is a fundamental ingredient in understanding a nucleus-nucleus collision. In order to study the nuclear potential, the colliding nuclei must be brought together close enough so that they experience the nuclear interaction. It has...
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フォーマット: | 学位論文 |
出版事項: |
2012
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オンライン・アクセス: | http://studentsrepo.um.edu.my/4139/1/Thesis.pdf http://studentsrepo.um.edu.my/4139/ |
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要約: | The knowledge of the nuclear potential between two colliding nuclei is a fundamental
ingredient in understanding a nucleus-nucleus collision. In order to
study the nuclear potential, the colliding nuclei must be brought together close
enough so that they experience the nuclear interaction. It has been demonstrated
that large-angle quasi-elastic scattering is a suitable method to study
the nuclear potential. In this thesis, analyses on the nuclear potential for heavyion
systems, namely 48Ti, 54Cr, 56Fe, 64Ni, and 70Zn + 208Pb systems, have been
performed through large-angle quasi-elastic scattering. At energies around the
Coulomb barrier height, it has been well known that the effect of channel couplings,
that is the coupling between the relative motion of the colliding nuclei
and their intrinsic motions as well as transfer processes, plays an important
role. Therefore, a coupled-channels procedure must be applied to take account
of this effect. cqel, which is a modified version of a computer code ccfull,
has been employed in order to perform these complex calculations. The nuclear
potential is assumed to have a Woods-Saxon form, which is characterized by
the surface diffuseness parameter, the potential depth, and the radius parameter.
It is found that low values of the diffuseness parameter in comparison with
the widely accepted value of around 0.63 fm are required in order to fit the
experimental data at deep sub-barrier energies, that is at energies well below
the Coulomb barrier height. In order to see the effect of collision energies on
the deduced values of the diffuseness parameter, experimental data with energies
up to 3 MeV below the Coulomb barrier height are used in the fittings.
This leads to higher deduced values of the diffuseness parameter, which are
closer to the widely accepted value. It seems that the phenomenon of threshold
anomaly might explain the relatively low diffuseness parameters obtained at
deep sub-barrier energies, and also the increase in the diffuseness parameters
as the collision energies increase. It is also possible that the increase in the
diffuseness parameters with respect to the energies is due to the same reasons
that might cause the diffuseness parameters obtained through fusion experimental
data higher than those obtained through scattering experimental data.
One of the possible reasons is the dynamical effects, particularly regarding the
neutron movements. Furthermore, the increase in the diffuseness parameters
as the collision energies are increased also seems to have a possible tendency to
be a function of the charge product of the target and projectile nuclei. |
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