On the Differential Cross Section for Neutron-Proton Scattering at 14.1 MeV

1974 ◽  
Vol 36 (2) ◽  
pp. 331-335 ◽  
Author(s):  
Shoji Shirato ◽  
Kazuo Saitoh
1963 ◽  
Vol 28 (5) ◽  
pp. 943-951 ◽  
Author(s):  
W. K. McFarlane ◽  
R. J. Homer ◽  
A. W. O’Dell ◽  
E. J. Sacharidis ◽  
G. H. Baton

2002 ◽  
Vol 80 (1) ◽  
pp. 39-42
Author(s):  
A Gashi ◽  
G Rasche ◽  
W S Woolcock

We give a compact expression for the unpolarized differential cross section for muon–proton scattering in the one-photon exchange approximation. The effect of adding the vacuum polarization amplitude to the no-spin-flip amplitude for one-photon exchange is calculated at small energies and scattering angles and is found to be negligible for present experiments. PACS No.: 13.6


1968 ◽  
Vol 4 (4) ◽  
pp. 353-373 ◽  
Author(s):  
G.F. Cox ◽  
G.H. Eaton ◽  
C.P. Van Zyl ◽  
O.N. Jarvis ◽  
B. Rose

The angular distribution for neutron-proton scattering at 156 ± 3 MeV has been determined for centre-of-mass scattering angles between 50 and 178°. The ratio σ(π) / σ (1/2 π ) is 5·0, and the minimum value of the differential cross-section occurs at an angle between 75 and 85°.


1980 ◽  
Vol 21 (4) ◽  
pp. 1185-1189 ◽  
Author(s):  
N. S. P. King ◽  
J. D. Reber ◽  
J. L. Romero ◽  
D. H. Fitzgerald ◽  
J. L. Ullmann ◽  
...  

2015 ◽  
Vol 30 (14) ◽  
pp. 1550076 ◽  
Author(s):  
F. Nemes ◽  
T. Csörgő ◽  
M. Csanád

The Bialas–Bzdak model of elastic proton–proton scattering assumes a purely imaginary forward scattering amplitude, which consequently vanishes at the diffractive minima. We extended the model to arbitrarily large real parts in a way that constraints from unitarity are satisfied. The resulting model is able to describe elastic pp scattering not only at the lower ISR energies but also at [Formula: see text] in a statistically acceptable manner, both in the diffractive cone and in the region of the first diffractive minimum. The total cross-section as well as the differential cross-section of elastic proton–proton scattering is predicted for the future LHC energies of [Formula: see text], 14, 15 TeV and also to 28 TeV. A nontrivial, significantly nonexponential feature of the differential cross-section of elastic proton–proton scattering is analyzed and the excitation function of the nonexponential behavior is predicted. The excitation function of the shadow profiles is discussed and related to saturation at small impact parameters.


1970 ◽  
Vol 28 (1) ◽  
pp. 11-15 ◽  
Author(s):  
Mitsuyoshi Tanaka ◽  
Norihiko Koori ◽  
Shoji Shirato

An external proton beam from the 110 in. Harwell cyclotron has been used to investigate proton-proton scattering at 147 MeV. The angular distribution of the scattering has been studied from 25 to 90° and found to be isotropic, within the limits of error. The absolute differential cross-section for scattering at 90° has been measured in two ways and found to be 4⋅94 ± 0⋅28 millibams. The results can also be used to find the 12 C( p , pn ) 11 C cross-section at 142 MeV.


2020 ◽  
Vol 84 (6) ◽  
pp. 747-750
Author(s):  
A. A. Terekhin ◽  
V. P. Ladygin ◽  
N. B. Ladygina ◽  
S. M. Piyadin ◽  
A. N. Khrenov ◽  
...  

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