Elastic and inelastic scattering in the 6Li, 9Be + 12C systems: excitation of unbound excited states and cluster transfers

1995 ◽  
Vol 591 (2) ◽  
pp. 349-370 ◽  
Author(s):  
J. Carter ◽  
Z.Z. Vilakazi ◽  
R.W. Fearick ◽  
V. Hnizdo ◽  
E. Muskat ◽  
...  
2016 ◽  
Vol 25 (10) ◽  
pp. 1650078 ◽  
Author(s):  
N. Burtebayev ◽  
S. K. Sakhiyev ◽  
D. M. Janseitov ◽  
Zh. Kerimkulov ◽  
D. Alimov ◽  
...  

We have measured the differential cross-sections for the elastic and inelastic scattering of [Formula: see text]-particles on [Formula: see text]C target at the isochronous cyclotron U-150 M INP Republic of Kazakhstan. The beam energies of [Formula: see text]-particles were 29[Formula: see text]MeV and 50[Formula: see text]MeV. As a result of research we obtained new experimental data for the [Formula: see text] + [Formula: see text]C elastic scattering and inelastic one leading to the 3.68 ([Formula: see text]), 6.86 ([Formula: see text]) and 7.5 ([Formula: see text])[Formula: see text]MeV excited states of [Formula: see text]C nucleus. The experimental results on elastic scattering were analyzed within the framework of the optical model using Woods–Saxon potential and the double folding one. The theoretical calculations for the concerned excited states were performed using the coupled channel (CC) method. The optimal deformation parameters for the excited states of [Formula: see text]C nucleus were extracted.


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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