Coupled Reaction Channels and Cluster Folding Analysis for 3He+20Ne Elastic and Inelastic Scattering

2019 ◽  
Vol 16 (6) ◽  
pp. 602-607
Author(s):  
Sh. Hamada
2021 ◽  
Vol 22 (1) ◽  
pp. 10-18
Author(s):  
A.T. Rudchik ◽  
◽  
A.A. Rudchik ◽  
O.E. Kutsyk ◽  
K. Rusek ◽  
...  

New experimental data of the 15N + 13C elastic and inelastic scattering were obtained at the energy Elab(15N) = 84 MeV. The data were analyzed within the coupled-reaction-channels method. The elastic and inelastic scattering of nuclei 15N + 13С as well as the more important nucleon and cluster transfer reactions were included in the channels-coupling scheme. The WS potential parameters for the 15N + 13С nuclei interactions in ground and excited states as well as deformation parameters of these nuclei were deduced. The contributions of one- and two-step transfers in the 15N + 13C elastic and inelastic scattering were estimated. The results of the 15N + 13С elastic scattering at the energy Elab(15N) = 84 MeV, obtained in this work, were compared with that of the 15N + 12С elastic scattering at the energy Elab(15N) = 81 MeV.


2005 ◽  
Vol 72 (3) ◽  
Author(s):  
A. A. Rudchik ◽  
A. T. Rudchik ◽  
G. M. Kozeratska ◽  
O. A. Ponkratenko ◽  
E. I. Koshchy ◽  
...  

Author(s):  
S. Golladay

The theory of multiple scattering has been worked out by Groves and comparisons have been made between predicted and observed signals for thick specimens observed in a STEM under conditions where phase contrast effects are unimportant. Independent measurements of the collection efficiencies of the two STEM detectors, calculations of the ratio σe/σi = R, where σe, σi are the total cross sections for elastic and inelastic scattering respectively, and a model of the unknown mass distribution are needed for these comparisons. In this paper an extension of this work will be described which allows the determination of the required efficiencies, R, and the unknown mass distribution from the data without additional measurements or models. Essential to the analysis is the fact that in a STEM two or more signal measurements can be made simultaneously at each image point.


1981 ◽  
Vol 102 (4) ◽  
pp. 242-246 ◽  
Author(s):  
M. Buenerd ◽  
J. Pinston ◽  
J. Cole ◽  
C. Guet ◽  
D. Lebrun ◽  
...  

1966 ◽  
Vol 79 (1) ◽  
pp. 188-192 ◽  
Author(s):  
I. Boca ◽  
M. Borşaru ◽  
M. Cenja ◽  
C. Haţegan ◽  
E. Iliescu ◽  
...  

1988 ◽  
Vol 489 (2) ◽  
pp. 329-346 ◽  
Author(s):  
W. Ott ◽  
R. Butsch ◽  
H.J. Jänsch ◽  
K.-H. Möbius ◽  
P. Paul ◽  
...  

1993 ◽  
Vol 553 ◽  
pp. 585-588 ◽  
Author(s):  
W.J. Briscoe ◽  
D.B. Barlow ◽  
B.L. Berman ◽  
R.W. Caress ◽  
K.S. Dhuga ◽  
...  

1969 ◽  
Vol 125 (3) ◽  
pp. 641-653 ◽  
Author(s):  
Kineo Tsukada ◽  
Shigeya Tanaka ◽  
Yoshiaki Tomita ◽  
Michio Maruyama

1976 ◽  
Vol 61 (4) ◽  
pp. 521-533 ◽  
Author(s):  
D. W. Glasgow ◽  
F. O. Purser ◽  
H. Hogue ◽  
J. C. Clement ◽  
K. Stelzer ◽  
...  

2014 ◽  
Vol 69 ◽  
pp. 00008 ◽  
Author(s):  
R. Capote ◽  
A. Trkov ◽  
M. Sin ◽  
M.W. Herman ◽  
E.Sh. Soukhovitskiĩ

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