The Fredholm determinant for Hulthén-distorted non-local separable potential: Application to $$ \alpha {-}\alpha $$ elastic scattering

Pramana ◽  
2020 ◽  
Vol 94 (1) ◽  
Author(s):  
U Laha ◽  
A K Behera ◽  
M Majumder ◽  
J Bhoi
1963 ◽  
Vol 18 (4) ◽  
pp. 531-538
Author(s):  
Dallas T. Hayes

Localized solutions of the BETHE—GOLDSTONE equation for two nucleons in nuclear matter are examined as a function of the center-of-mass momentum (c. m. m.) of the two nucleons. The equation depends upon the c. m. m. as parameter due to the dependence upon the c. m. m. of the projection operator appearing in the equation. An analytical solution of the equation is obtained for a non-local but separable potential, whereby a numerical solution is also obtained. An approximate solution for small c. m. m. is calculated for a square-well potential. In the range of the approximation the two analytical solutions agree exactly.


1970 ◽  
Vol 148 (2) ◽  
pp. 391-400 ◽  
Author(s):  
W. Grüebler ◽  
V. König ◽  
P.A. Schmelzbach ◽  
P. Marmier

Author(s):  
H.N. Tran ◽  
Z. El Bitar ◽  
C. Champion ◽  
M. Karamitros ◽  
M.A. Bernal ◽  
...  

2016 ◽  
Vol 94 (1) ◽  
pp. 95-101 ◽  
Author(s):  
Z.F. Shehadeh

The differential and reaction cross sections for alpha–alpha elastic scattering at energies ranging from 50 to 120 MeV (lab. system) have been clearly explained for the first time, by using a new optical potential type. This potential, which is different from all other proposed potentials, is composed of two real parts: one is an attractive squared Woods–Saxon and the other is a repulsive core of the Woods–Saxon form in addition to a surface Woods–Saxon form for the imaginary part. The nature of the real part has been determined from available phase shifts through using inverse scattering theory for the identical particles at a fixed energy, adopting the framework of the Schrödinger equation. It is found that the repulsive real part is essential for improving the fit to the measured elastic differential cross sections, and in explaining the kink that appears at r < 1.0 fm in the shape of the real part of the potential. Using this new potential, our calculated reaction cross sections are in reasonable agreement with the ones reported by both Darriulat et al. (Phys. Rev. 137, B315 (1965). doi:10.1103/PhysRev.137.B315) and Brown and Tang (Nucl. Phys. A, 170, 225 (1971). doi:10.1016/0375-9474(71)90633-6 ).


1985 ◽  
Vol 152 (1-2) ◽  
pp. 140-144 ◽  
Author(s):  
T. Åkesson ◽  
M.G. Albrow ◽  
S. Almehed ◽  
R. Batley ◽  
O. Benary ◽  
...  

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