“…The parameters V Y , W Y and α 2 of the Gaussian potential, equation (21), are used as free parameters to fit the measured NN scattering values of σ, ρ, and β NN [49,50]. The results of these calculations are given in table 4.…”
“…Theoretically, the medium NN cross section can be calculated by solving the many-body Bethe-Goldstone (BG) equation, namely G matrix cross section [13,14]. Many authors [15][16][17][18][19][20][21][22] have studied medium effect of NN cross section. Based upon the Bonn A NN interactive potential and Dirac-Brueckner approach for nuclear matter, in-medium NN cross sections were calculated by Li and Machleidt [15,16] for the incident energies from 50 to 300 MeV in a laboratory frame.…”
Analytical formulae are used to calculate the phase variation and the slope parameter of the nucleon–nucleon (NN) scattering amplitude in terms of momentum transfer q2. An empirical series is presented to calculate the total NN cross section. The proton–nucleus and nucleus–nucleus elastic differential cross–sections for different reactions at different bombarding energies less than 200 MeV/N have been calculated. The phase variation and the in-medium effect are considered in these calculations using the Glauber model. The calculated cross sections are in reasonable agreement with the experimental data over the whole range of energy considered in this work among light and medium nuclei.
“…The parameters V Y , W Y and α 2 of the Gaussian potential, equation (21), are used as free parameters to fit the measured NN scattering values of σ, ρ, and β NN [49,50]. The results of these calculations are given in table 4.…”
“…Theoretically, the medium NN cross section can be calculated by solving the many-body Bethe-Goldstone (BG) equation, namely G matrix cross section [13,14]. Many authors [15][16][17][18][19][20][21][22] have studied medium effect of NN cross section. Based upon the Bonn A NN interactive potential and Dirac-Brueckner approach for nuclear matter, in-medium NN cross sections were calculated by Li and Machleidt [15,16] for the incident energies from 50 to 300 MeV in a laboratory frame.…”
Analytical formulae are used to calculate the phase variation and the slope parameter of the nucleon–nucleon (NN) scattering amplitude in terms of momentum transfer q2. An empirical series is presented to calculate the total NN cross section. The proton–nucleus and nucleus–nucleus elastic differential cross–sections for different reactions at different bombarding energies less than 200 MeV/N have been calculated. The phase variation and the in-medium effect are considered in these calculations using the Glauber model. The calculated cross sections are in reasonable agreement with the experimental data over the whole range of energy considered in this work among light and medium nuclei.
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