scholarly journals One-pion-exchange potential with contact terms from lattice QCD simulations

2020 ◽  
Vol 44 (7) ◽  
pp. 071002
Author(s):  
Jinniu Hu ◽  
Ying Zhang ◽  
Hong Shen ◽  
Hiroshi Toki
1993 ◽  
Vol 46 (6) ◽  
pp. 737
Author(s):  
GQ Liu ◽  
AW Thomas

To distinguish explicit quark effects from meson exchange in the NN interaction, it is necessary to splice the long-range meson exchange forces and short-distance dynamics due to quarks. However, in most quark model studies the short-range part of the pion exchange is usually treated differently, which makes it difficult to get a uniform picture of the short-range dynamics. We make a comparison between meson exchange and quark-gluon dynamics using the same pion exchange potential based on a quark-pion coupling model. The roles of vector meson exchange and gluon exchange in the NN interaction are compared by calculating NN phase parameters. It is shown that, with this consistent one-pion exchange force, the vector meson exchange gives a better fit to the data. This suggests that non-perturbative mechanisms responsible for meson exchange may need more careful handling to supplement the usual one-gluon exchange mechanism in describing the NN interaction.


1957 ◽  
Vol 107 (1) ◽  
pp. 320-321 ◽  
Author(s):  
Michiji Konuma ◽  
Hironari Miyazawa ◽  
Shoichiro Otsuki

1984 ◽  
Vol 30 (3) ◽  
pp. 1084-1086 ◽  
Author(s):  
J. L. Friar ◽  
B. F. Gibson ◽  
G. L. Payne

1993 ◽  
Vol 48 (2) ◽  
pp. 920-923 ◽  
Author(s):  
O. L. Battistel ◽  
M. R. Robilotta

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.


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