scholarly journals Proton elastic scattering from tin isotopes at 295 MeV and systematic change of neutron density distributions

2008 ◽  
Vol 77 (2) ◽  
Author(s):  
S. Terashima ◽  
H. Sakaguchi ◽  
H. Takeda ◽  
T. Ishikawa ◽  
M. Itoh ◽  
...  
Keyword(s):  
Elastic Scattering ◽  
Systematic Change ◽  
Neutron Density ◽  
Density Distributions ◽  
Proton Elastic Scattering

Neutron density distributions ofPb204,206,208deduced via proton elastic scattering atEp=295MeV

2010 ◽  
Vol 82 (4) ◽  
Author(s):  
J. Zenihiro ◽  
H. Sakaguchi ◽  
T. Murakami ◽  
M. Yosoi ◽  
Y. Yasuda ◽  
...  
Keyword(s):  
Elastic Scattering ◽  
Neutron Density ◽  
Density Distributions ◽  
Proton Elastic Scattering

scholarly journals PROTON ELASTIC SCATTERING AND NEUTRON DISTRIBUTION OF UNSTABLE NUCLEI

1999 ◽  
Vol 08 (02) ◽  
pp. 167-178 ◽  
Author(s):  
K. KAKI ◽  
S. HIRENZAKI
Keyword(s):  
Elastic Scattering ◽  
Scattering Data ◽  
Neutron Density ◽  
Neutron Distribution ◽  
Density Distributions ◽  
Proton Elastic Scattering ◽  
Unstable Nuclei ◽  
Impulse Model

We study theoretically how we can determine the neutron density distributions of unstable nuclei from proton elastic scattering. We apply the relativistic impulse model to study the sensitivities of the observables to the density distributions which are expressed in Woods-Saxon form. We find that both the radius and diffuseness of densities can be determined from restricted elastic scattering data in principle. We think this result is helpful to design future experiments.

Elastic scattering analysis of p+40Ca at incident energies from threshold to 48.4 MeV and nuclear matter radius

2015 ◽  
Vol 24 (07) ◽  
pp. 1550055
Author(s):  
Atef Ismail ◽  
Yen Cheong Lee ◽  
M Tammam
Keyword(s):  
Elastic Scattering ◽  
Cross Sections ◽  
Theoretical Calculations ◽  
Reaction Cross ◽  
Angular Distributions ◽  
Folding Potential ◽  
Density Distributions ◽  
Proton Elastic Scattering ◽  
Broad Energy Range ◽  
Broad Energy

Proton elastic scattering at various incident energies is one method to study nuclear density distributions and nuclear radii. Single folding potential describing the p-scattering on 40 Ca over a broad energy range 9–48.4 MeV is constructed. The resulting potential does not need any renormalization to fit the measured elastic scattering angular distributions and total reaction cross-sections. Furthermore, correlation between volume integral and proton incident energy is discussed. Theoretical calculations are in a good agreement with existing experimental data.

Neutron density distributions analyzed in terms of relativistic impulse approximation for nickel isotopes

2015 ◽  
Vol 24 (03) ◽  
pp. 1550015 ◽  
Author(s):  
Kaori Kaki
Keyword(s):  
Form Factor ◽  
Elastic Scattering ◽  
Cross Section ◽  
Impulse Approximation ◽  
Model Analysis ◽  
Medium Effect ◽  
Neutron Density ◽  
Neutron Distribution ◽  
Density Distributions ◽  
Nickel Isotopes

Observables of proton elastic scattering from nickel isotopes (48–82 Ni ) are calculated based on relativistic impulse approximation (RIA), and nuclear density distributions are provided by relativistic mean-field (RMF) calculations. Contributions of a medium effect and multiple scattering to observables are evaluated and shown to be small at incident proton energies from 200 MeV through 500 MeV so that it is confirmed to perform a model analysis based on the fundamental RIA calculation. For 58,60,62,64 Ni isotopes, are considered proton distributions which are obtained by means of unfolding the charge form factor of proton from charge densities determined by the experiments of electron scattering. Through comparisons between results for the different proton densities, contributions of proton form factor to proton distributions and to elastic scattering observables at 300 MeV are discussed. It is shown that the neutron distribution is determined from the restricted observables, reaction cross-section and the first dip of differential cross-section, based on a model analysis of Woods–Saxon distribution in the case of 64 Ni target at 300 MeV. Contributions of tensor density and empirical proton density are shown to obtaining the neutron distribution with the model analysis. Compared with the similar studies for 40,60 Ca and 208 Pb , problems of the model analysis, which arise out of errors in observables, are discussed.

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