Proton elastic scattering on light nuclei. II. Nuclear structure effects

1980 ◽  
Vol 21 (3) ◽  
pp. 844-860 ◽  
Author(s):  
E. Fabrici ◽  
S. Micheletti ◽  
M. Pignanelli ◽  
F. G. Resmini ◽  
R. De Leo ◽  
...  
1974 ◽  
Vol 10 (5) ◽  
pp. 1678-1687 ◽  
Author(s):  
J. C. Manthuruthil ◽  
C. P. Poirier ◽  
S. Maripuu ◽  
W. A. Anderson

1976 ◽  
Vol 36 (23) ◽  
pp. 1357-1359 ◽  
Author(s):  
P. G. Ikossi ◽  
W. J. Thompson ◽  
T. B. Clegg ◽  
W. W. Jacobs ◽  
E. J. Ludwig

1977 ◽  
Vol 30 (3) ◽  
pp. 287 ◽  
Author(s):  
A Gabric ◽  
K Amos

Allowing for important doorway state effects in analyses of proton elastic scattering from the light nuclei 14N and 160 enables an average geometry optical model potential to be determined, the strength parameters of which show a smooth behaviour with projectile energy.


1980 ◽  
Vol 21 (3) ◽  
pp. 830-843 ◽  
Author(s):  
E. Fabrici ◽  
S. Micheletti ◽  
M. Pignanelli ◽  
F. G. Resmini ◽  
R. De Leo ◽  
...  

2020 ◽  
Vol 31 (1) ◽  
Author(s):  
Huan Nhut Phan

Nuclear reactions of proton by light nuclei at low energies play a key role in the study ofnucleosynthesis which is of interest in nuclear astrophysics. The most fundamental process whichis very necessary is the elastic scattering. In this work, we construct a microscopic proton-nucleuspotential in order to describe the differential cross-sections over scattering angles of the protonelastic scattering by 12C and 13C in the range of available energies 14 - 22 MeV. The microscopicoptical potential is based on the folding model using the effective nucleon-nucleon interactionCDM3Yn. The results show the promising use of the CDM3Yn interactions at low and very lowenergies, which were originally used for nuclear reactions at intermediate energies. This could bethe premise for the study of nuclear reactions using CDM3Yn interaction in astrophysics at lowenergies.


2022 ◽  
Vol 63 (1) ◽  
Author(s):  
Ch. Elster ◽  
M. Burrows ◽  
R. B. Baker ◽  
S. P. Weppner ◽  
K. D. Launey ◽  
...  

Author(s):  
Roger H. Stuewer

Serious contradictions to the existence of electrons in nuclei impinged in one way or another on the theory of beta decay and became acute when Charles Ellis and William Wooster proved, in an experimental tour de force in 1927, that beta particles are emitted from a radioactive nucleus with a continuous distribution of energies. Bohr concluded that energy is not conserved in the nucleus, an idea that Wolfgang Pauli vigorously opposed. Another puzzle arose in alpha-particle experiments. Walther Bothe and his co-workers used his coincidence method in 1928–30 and concluded that energetic gamma rays are produced when polonium alpha particles bombard beryllium and other light nuclei. That stimulated Frédéric Joliot and Irène Curie to carry out related experiments. These experimental results were thoroughly discussed at a conference that Enrico Fermi organized in Rome in October 1931, whose proceedings included the first publication of Pauli’s neutrino hypothesis.


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