On the geometrical shape of the single particle spin-orbit potential

1985 ◽  
Vol 322 (4) ◽  
pp. 665-667 ◽  
Author(s):  
R. Bhattacharya
1972 ◽  
Vol 27 (5) ◽  
pp. 863-864
Author(s):  
R Penzel ◽  
W Stocker

Abstract The exchange part of the single-particle spin-orbit potential following from a two-body spin-orbit potential is calculated. Scheerbaum's approximation of setting the exchange part equal to the direct part is investigated


1979 ◽  
Vol 83 (3-4) ◽  
pp. 279-283 ◽  
Author(s):  
Y. Tanaka ◽  
Y. Oda ◽  
F. Petrovich ◽  
R.K. Sheline

2000 ◽  
Vol 674 (3-4) ◽  
pp. 493-514 ◽  
Author(s):  
Y. Fujiwara ◽  
M. Kohno ◽  
T. Fujita ◽  
C. Nakamoto ◽  
Y. Suzuki

1981 ◽  
Vol 66 (1) ◽  
pp. 227-250 ◽  
Author(s):  
K. Ando ◽  
H. Bando

2016 ◽  
Vol 25 (08) ◽  
pp. 1650055 ◽  
Author(s):  
J. A. Liendo ◽  
E. Castro ◽  
R. Gómez ◽  
D. D. Caussyn

The experimental binding energies of single-particle and single-hole neutron states belonging to neutron shells that extend from [Formula: see text] = 126–184 and 82–126, respectively, have been reproduced by solving the Schrödinger equation with a potential that has two components: the generalized Woods–Saxon (GWS) potential and the spin-orbit (SO) coupling term. The GWS potential contains the traditional WS potential plus a term (SU) whose intensity reaches a maximum in the nuclear surface. Our results indicate the existence of an explicit relationship between the strength of the SU potential and the orbital angular momentum quantum number [Formula: see text] of the state. This dependence has been used to make reasonable predictions for the excitation energy centroids of states located inside and outside the neutron shells investigated. Comparisons are made with results reported in previous investigations.


2000 ◽  
Vol 670 (1-4) ◽  
pp. 319-322 ◽  
Author(s):  
M. Kohno ◽  
Y. Fujiwara ◽  
T. Fujita ◽  
C. Nakamoto ◽  
Y. Suzuki

1960 ◽  
Vol 76 (6) ◽  
pp. 1002-1002
Author(s):  
D W L Sprung ◽  
J B Willis

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