Systematic model-independent S -matrix analysis of He4−Ca40 elastic scattering in going from anomalous large-angle scattering to near-Coulomb-barrier scattering

2018 ◽  
Vol 97 (3) ◽  
Author(s):  
V. Yu. Korda ◽  
A. S. Molev ◽  
L. P. Korda ◽  
V. F. Klepikov

The results of the investigation of the angular distributions of electrons scattered elastically and inelastically in helium, argon, and mercury vapour have been described in a previous paper. It was found that the inelastic angular distributions in mercury vapour and argon exhibited diffraction maxima and minima similar to those which appeared in the elastic angular distributions. Recently Tate and Palmer have investigated the elastic scattering in mercury vapour for angles of scattering between 5° and 125°, and the inelastic scattering (corresponding to a discrete energy loss) between 5° and 55°. Hughes and McMillen have measured the angular distributions of the elastic and inelastic scattering in hydrogen between 40° and 165°, and the elastic scattering in helium between 15° and 150°. These papers are also concerned with the large angle scattering of those electrons which make ionising collisions.



Author(s):  
R. B. Galloway

SynopsisThe state of knowledge of fast neutron polarisation due to elastic scattering is reviewed in relation to the optical model of the process. There is clearly a substantial lack of polarisation data at neutron energies and concerning nuclei appropriate to the optical model description. The situation for the extremes of small and of large angle scattering is also considered.



1960 ◽  
Vol 117 (1) ◽  
pp. 247-249 ◽  
Author(s):  
J. L. Lloyd ◽  
A. W. Wolfendale


1965 ◽  
Vol 18 (2) ◽  
pp. 195-196 ◽  
Author(s):  
S.P. Alliluyev ◽  
S.S. Gershtein ◽  
A.A. Logunov




1979 ◽  
Vol 24 (4) ◽  
pp. 110-114 ◽  
Author(s):  
S. V. Goloskokov ◽  
A. V. Koudinov ◽  
S. P. Kuleshov


1969 ◽  
Vol 4 (6) ◽  
pp. 347-348 ◽  
Author(s):  
M. Fink ◽  
R.A. Bonham ◽  
J.S. Lee ◽  
E.W. Ng


Author(s):  
N. F. Mott

1. The formulae usually given for the scattering of electrons by atoms are calculated without taking into account the radiative forces. It has been suggested by the author in a former paper that in the case of the large-angle scattering of electrons with velocity comparable with that of light (for which case the scattering is entirely nuclear), these forces might influence the scattering by an appreciable amount, which would explain the divergence between the theoretical formula and the results of Chadwick and Mercier, which are some 40 per cent. greater. In this paper we shall show that for electrons–of any velocity the influence of these forces cannot be greater than 2 or 3 per cent., and so cannot be invoked to explain discrepancies between theory and experiment.



1980 ◽  
Vol 21 (6) ◽  
pp. 1891-1901 ◽  
Author(s):  
H. H. Andersen ◽  
F. Besenbacher ◽  
P. Loftager ◽  
W. Möller


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