Coulomb effect on the proton-proton low-energy scattering parameters

1970 ◽  
Vol 141 (2) ◽  
pp. 369-374 ◽  
Author(s):  
Vo-Dai Thien ◽  
Y. Nogami
1975 ◽  
Vol 53 (18) ◽  
pp. 1779-1779
Author(s):  
M. W. Kermode ◽  
Y. Nogami ◽  
W. Van Dijk

1986 ◽  
Vol 33 (6) ◽  
pp. 3749-3755 ◽  
Author(s):  
L. P. Benofy ◽  
E. Buendía ◽  
R. Guardiola ◽  
M. de Llano

1975 ◽  
Vol 53 (3) ◽  
pp. 207-209 ◽  
Author(s):  
M. W. Kermode ◽  
Y. Nogami ◽  
W. van Dijk

The effect of the Coulomb force on low energy proton–proton scattering is examined when the nuclear interaction is represented by a rank one separable potential of Tabakin's type. The scattering length which is obtained by switching off the Coulomb force is found to be −20.0 F. This value is appreciably different from those for local realistic potentials. This anomaly is similar to the one which was recently found by Sauer.


2017 ◽  
Vol 48 (10) ◽  
pp. 1801 ◽  
Author(s):  
T. Ishikawa ◽  
K. Aoki ◽  
H. Fujioka ◽  
Y. Honda ◽  
T. Hotta ◽  
...  

1960 ◽  
Vol 31 (12) ◽  
pp. 2104-2111 ◽  
Author(s):  
Larry Spruch ◽  
Leonard Rosenberg

2020 ◽  
Vol 56 (9) ◽  
Author(s):  
Gábor Balassa ◽  
György Wolf

Abstract In this work, we extended our statistical model with charmed and bottomed hadrons, and fit the quark creational probabilities for the heavy quarks, using low energy inclusive charmonium and bottomonium data. With the finalized fit for all the relevant types of quarks (up, down, strange, charm, bottom) at the energy range from a few GeV up to a few tens of GeV’s, the model is now considered complete. Some examples are also given for proton–proton, pion–proton, and proton–antiproton collisions with charmonium, bottomonium, and open charm hadrons in the final state.


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