Elastic Scattering of Intermediate-Energy Alpha Particles by Gold

1954 ◽  
Vol 93 (2) ◽  
pp. 356-357 ◽  
Author(s):  
George W. Farwell ◽  
Harvey E. Wegner
1994 ◽  
Vol 49 (3) ◽  
pp. 1609-1620 ◽  
Author(s):  
Anders Ingemarsson ◽  
Agris Auce ◽  
Roger Johansson

1954 ◽  
Vol 95 (5) ◽  
pp. 1212-1217 ◽  
Author(s):  
George W. Farwell ◽  
Harvey E. Wegner

2001 ◽  
Vol 684 (1-4) ◽  
pp. 580-582 ◽  
Author(s):  
N. Kalantar-Nayestanaki ◽  
R. Bieber ◽  
W. Glöckle ◽  
J. Golak ◽  
M.N. Harakeh ◽  
...  

1961 ◽  
Vol 122 (1) ◽  
pp. 232-241 ◽  
Author(s):  
H. Smotrich ◽  
K. W. Jones ◽  
L. C. McDermott ◽  
R. E. Benenson

1991 ◽  
Vol 43 (4) ◽  
pp. 1867-1874 ◽  
Author(s):  
P. Singh ◽  
A. Chatterjee ◽  
S. K. Gupta ◽  
S. S. Kerekatte

2020 ◽  
Vol 56 (12) ◽  
Author(s):  
Pierre Capel ◽  
Ronald C. Johnson ◽  
Filomena M. Nunes

AbstractFor one-neutron halo nuclei, the cross sections for elastic scattering and breakup at intermediate energy exhibit similar angular dependences. The Recoil Excitation and Breakup (REB) model of reactions elegantly explains this feature. It also leads to the idea of a new reaction observable to study the structure of loosely-bound nuclear systems: the Ratio. This observable consists of the ratio of angular distributions for different reaction channels, viz. elastic scattering and breakup, which cancels most of the dependence on the reaction mechanism; in particular it is insensitive to the choice of optical potentials that simulate the projectile-target interaction. This new observable is very sensitive to the structure of the projectile. In this article, we review a series of previous papers, which have introduced the Ratio Method and its extension to low beam energies and proton-halo nuclei.


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