Phase variation of the nucleon-nucleon amplitude and the spin observables in proton−4He elastic scattering

1990 ◽  
Vol 41 (4) ◽  
pp. R1348-R1350 ◽  
Author(s):  
R. J. Lombard ◽  
J. P. Maillet
2020 ◽  
Vol 95 (9) ◽  
pp. 095301
Author(s):  
M Y H Farag ◽  
I I A Bashter ◽  
I A M Abdul-Magead ◽  
M M H El-Azony

2014 ◽  
Vol 23 (03) ◽  
pp. 1450010 ◽  
Author(s):  
Ibrahim M. A. Tag El-Din ◽  
M. M. Taha ◽  
Samia S. A. Hassan

The total nuclear reaction cross-section σRfor p-4He in the energy range from 25 MeV to 1000 MeV is calculated within Glauber and Coulomb-modified Glauber models. The Coulomb-modified Glauber model (CMGM) is introduced via modification of the Coulomb trajectory of the projectile from a straight line, and calculation of the effective radius of interaction. The effects of in-medium nucleon–nucleon (NN) total cross-section, phase variation, high order momentum transfer component of nucleon–nucleon elastic scattering amplitude and Pauli blocking are studied. It is pointed out that the phase variation of the nucleon–nucleon amplitude plays a significant role in describing σRwith γ = -1.6 fm2at in-medium nuclear density ϱ = 0 and γ = -2 fm2at ϱ = 0.17 fm-3in the whole energy range. A remarkable fit to the available experimental data is obtained by invoking Pauli blocking and high order momentum transfer of nucleon–nucleon (NN) elastic scattering amplitude for Ep< 100 MeV.


1996 ◽  
Vol 49 (3) ◽  
pp. 655 ◽  
Author(s):  
Mohamed A Hassan ◽  
Hamed EA Awd-Allah ◽  
Samia SA Hassan ◽  
Ibrahim MA Tag El-Din

Proton–deuteron elastic scattering at intermediate and high energies illustrates the importance of the phase variation of the nucleon–nucleon elastic scattering amplitude as in previous work. Two kinds of phase variation are examined. The first is the usual one which is related to free nucleon-free nucleon collisions as suggested by Franco. The second is assumed to be related to the time ordering of multi-scattering processes. The two kinds play similar roles in improving the results. The contributions of both kinds lead to a good fit to the experimental data at the energies considered. The value of the phase variation parameter in each kind (where they are considered together), which gives a good fit to the experimental data, are approximately the same and of order 4 (GeV / c)‾ 2. Also, with relatively small values of the phase variation parameter, the phase variation effect improves the agreement with the experimental data for the p–4He elastic scattering differential cross section at the minimum region in the energy range 97–393 GeV.


1987 ◽  
Vol 36 (5) ◽  
pp. 2010-2017 ◽  
Author(s):  
M. Haji-Saied ◽  
E. Bleszynski ◽  
M. Bleszynski ◽  
J. Carroll ◽  
G. J. Igo ◽  
...  

1991 ◽  
Vol 17 (12) ◽  
pp. 1823-1831 ◽  
Author(s):  
R J Lombard ◽  
J P Maillet ◽  
J Van de Wiele

1978 ◽  
Vol 17 (7) ◽  
pp. 1709-1712 ◽  
Author(s):  
S. L. Kramer ◽  
D. S. Ayres ◽  
D. Cohen ◽  
R. Diebold ◽  
A. J. Pawlicki ◽  
...  

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