Measurement and Statistical Theory Analysis ofFe56(He3, p)andCu63(He3, p)Energy and Angular Distributions-Nuclear Shell Effects

1965 ◽  
Vol 139 (4B) ◽  
pp. B835-B845 ◽  
Author(s):  
Jean-Pierre Hazan ◽  
George Merkel
1986 ◽  
Vol 96 (4) ◽  
pp. 323-338 ◽  
Author(s):  
R. Guidotti ◽  
F. Saporetti ◽  
G. Maino ◽  
A. Ventura

2001 ◽  
Vol 688 (1-2) ◽  
pp. 353-356 ◽  
Author(s):  
M.M. Sharma ◽  
A.R. Farhan

2009 ◽  
Vol 18 (10) ◽  
pp. 2155-2159
Author(s):  
J. DUDEK ◽  
D. CURIEN ◽  
A. GÓŹDŹ ◽  
K. MAZUREK

The nuclear mean-field theory and the group representation theory can be used to optimise the search for strong nuclear shell effects. The two theories allow to correlate the symmetry aspects with the presence of large gaps in the single-particle spectra, facilitate in this way the conditions of search for strong nucleonic- and nuclear-binding and thus for an increased nuclear stability. In this article we give a short overview of the related on-going research, focussing on the results of the TetraNuc Collaboration.


2015 ◽  
Vol 91 (4) ◽  
Author(s):  
A. Chaudhuri ◽  
T. K. Ghosh ◽  
K. Banerjee ◽  
S. Bhattacharya ◽  
Jhilam Sadhukhan ◽  
...  

Science ◽  
2012 ◽  
Vol 337 (6099) ◽  
pp. 1207-1210 ◽  
Author(s):  
E. M. Ramirez ◽  
D. Ackermann ◽  
K. Blaum ◽  
M. Block ◽  
C. Droese ◽  
...  

2004 ◽  
Vol 13 (05) ◽  
pp. 987-997 ◽  
Author(s):  
S. ADHIKARI ◽  
C. SAMANTA

The variation of nuclear shell effects with nucleon numbers is evaluated using the modified Bethe–Weizsäcker mass formula (BWM) and the measured atomic masses. The shell effects at magic neutron numbers N=8, 20, 28, 50, 82 and 126 and magic proton numbers Z=8, 20, 28, 50 and 82 are found to vary rapidly approaching the drip-lines. The shell effect due to one magic number increases on approaching another magic number. Thus, shell effects are not always negligible near the drip-lines.


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