Energy dependence of 12C+12C single-neutron transfer cross sections

1988 ◽  
Vol 203 (4) ◽  
pp. 345-348 ◽  
Author(s):  
J.S. Winfield ◽  
Sam M. Austin ◽  
G.M. Crawley ◽  
C. Djalali ◽  
C.A. Ogilvie ◽  
...  
1973 ◽  
Vol 51 (18) ◽  
pp. 2000-2022 ◽  
Author(s):  
D. E. Nelson ◽  
D. G. Burke ◽  
J. C. Waddington ◽  
W. B. Cook

Properties of nuclear levels in 151Sm have been studied by measuring angular distributions for the 152Sm(d,t)151Sm reaction and spectra at several angles for the 152Sm(3He,α)151Sm and 150Sm(d,p)151Sm reactions. The reaction products were analyzed with a magnetic spectrograph and detected with photographic emulsions. Transfer l values were deduced from the (d,t) angular distributions and from the ratios of (3He,α) and (d,t) cross sections. The (d,t), (d,p), and (3He,α) reactions on targets of 151Sm were also studied in order to learn more about the wave function of the 151Sm ground state. The low-lying positive parity levels can be described by the Nilsson model with Coriolis and ΔN = 2 interactions included. However, the properties of the low energy negative parity states could not be explained as easily. No mixture of Nilsson states was found which could simultaneously explain the single neutron transfer intensities and the Coulomb excitation probabilities from previous measurements.


2019 ◽  
Vol 34 (32) ◽  
pp. 1950259 ◽  
Author(s):  
S. M. Troshin ◽  
N. E. Tyurin

We comment briefly on relations between the elastic and inelastic cross-sections valid for the shadow and reflective modes of the elastic scattering. Those are based on the unitarity arguments. It is shown that the redistribution of the probabilities of the elastic and inelastic interactions (the form of the inelastic overlap function becomes peripheral) under the reflective scattering mode can lead to increasing ratio of [Formula: see text] at the LHC energies. In the shadow scattering mode, the mechanism of this increase is a different one, since the impact parameter dependence of the inelastic interactions probability is central in this mode. A short notice is also given on the slope parameter and the leading contributions to its energy dependence in both modes.


1996 ◽  
Vol 53 (4) ◽  
pp. 2337-2344 ◽  
Author(s):  
J.-Y. Chesnel ◽  
H. Merabet ◽  
X. Husson ◽  
F. Frémont ◽  
D. Lecler ◽  
...  

1985 ◽  
Vol 445 (4) ◽  
pp. 669-684 ◽  
Author(s):  
M. Garçon ◽  
D. Legrand ◽  
R.M. Lombard ◽  
B. Mayer ◽  
M. Rouger ◽  
...  

Exotic Nuclei ◽  
2017 ◽  
Author(s):  
Yu. E. Penionzhkevich ◽  
Yu. G. Sobolev ◽  
V. V. Samarin ◽  
M. A. Naumenko

1987 ◽  
Vol 48 (11) ◽  
pp. 1901-1924 ◽  
Author(s):  
J. Bystricky ◽  
P. La France ◽  
F. Lehar ◽  
F. Perrot ◽  
T. Siemiarczuk ◽  
...  

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