Form of the One-Pion Exchange Potential

1960 ◽  
Vol 5 (6) ◽  
pp. 274-276 ◽  
Author(s):  
G. Breit ◽  
M. H. Hull ◽  
K. Lassila ◽  
H. M. Ruppel
2014 ◽  
Vol 29 ◽  
pp. 1460226
Author(s):  
Y. Yamaguchi ◽  
A. Hosaka ◽  
S. Yasui

We discuss the possible existence of exotic dibaryons with a heavy antiquark, being realized three-body systems, [Formula: see text] and B(*)NN. These are genuinely exotic states with no quark-antiquark annihilation. We consider the heavy quark spin symmetry and chiral symmetry, and introduce the one pion exchange potential between a [Formula: see text] meson and a nucleon N. As for the NN interaction, we employ the Argonne [Formula: see text] potential. By solving the coupled-channel equations for PNN and [Formula: see text], we find bound and resonant states near the thresholds both in charm and bottom sectors.


1993 ◽  
Vol 47 (2) ◽  
pp. 877-880 ◽  
Author(s):  
Zhi-Xin Qian ◽  
Cheng-Gang Su ◽  
Ru-Keng Su

1960 ◽  
Vol 46 (12) ◽  
pp. 1649-1657 ◽  
Author(s):  
G. Breit ◽  
M. H. Hull ◽  
K. E. Lassila ◽  
H. M. Ruppel

1973 ◽  
Vol 6 (16) ◽  
pp. 663-667 ◽  
Author(s):  
P. Calogero ◽  
P. Palumbo

1992 ◽  
Vol 01 (01) ◽  
pp. 201-213 ◽  
Author(s):  
B. K. JAIN ◽  
A. B. SANTRA

Considering that, in pp scattering, the pp → n Δ++ transition occurs mainly from the elastic channel, a t-matrix for this process was constructed by us earlier. This t-matrix describes the measured cross-sections on the p (p, n) Δ++ process very well from threshold to a few GeV. The transition potential in it is described by the one pion-exchange potential and the elastic scattering wave function through the "measured" elastic scattering amplitude. In this paper, we have parametrized this t-matrix so that it can be used for describing the (p, Δ++) reaction in nuclei. The parametrized t-matrix has been found to have a structure similar to one pion-exchange potential except that it has a softer form factor (Λ ≈ 650–800 MeV/c ) and it has a Migdal term (g′ ≈ 0.65) in the central term. The imaginary part of the t-matrix is weak. In the single scattering approximation this t-matrix describes the measured cross-sections on p(3 He , t) Δ++ and 6 Li (p, Δ++)6 He reactions very well. It is also found that with this t-matrix, the "projectile excitation" contribution to the reaction is small.


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