Energy Dependence of Elastic and Inelastic Scattering fromC12for Protons between 14 and 19 MeV

1964 ◽  
Vol 133 (4B) ◽  
pp. B934-B947 ◽  
Author(s):  
W. W. Daehnick ◽  
R. Sherr
2020 ◽  
Vol 35 (19) ◽  
pp. 2050159
Author(s):  
Yu. A. Berezhnoy ◽  
A. S. Molev

We present the results of the [Formula: see text]-matrix description of the [Formula: see text] elastic and inelastic scattering differential cross-sections between 40 and 240 MeV with allocation of Airy minima of various orders. The first-order Airy minima have been unambiguously identified in the differential cross-sections for elastic scattering and inelastic scattering to the first [Formula: see text] state of [Formula: see text] at energies [Formula: see text] MeV, and the second-order Airy minima — at [Formula: see text] MeV. The angular positions of these minima obey an inverse dependence on energy. The intensities of nuclear refraction and absorption also obey the same energy dependence.


1964 ◽  
Vol 135 (3B) ◽  
pp. B660-B668 ◽  
Author(s):  
R. A. Atneosen ◽  
H. L. Wilson ◽  
M. B. Sampson ◽  
D. W. Miller

1977 ◽  
Vol 292 (1-2) ◽  
pp. 1-19 ◽  
Author(s):  
O. Karban ◽  
W.E. Burcham ◽  
J.B.A. England ◽  
R.G. Harris ◽  
S. Roman

1985 ◽  
Vol 155 (1-2) ◽  
pp. 27-30 ◽  
Author(s):  
P.H. Kutt ◽  
S.F. Pate ◽  
A.H. Wuosmaa ◽  
R.W. Zurmühle ◽  
Ole Hansen ◽  
...  

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 ◽  
...  

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