BARYON–BARYON INTERACTION IN THE EXTENDED CHIRAL SU(3) QUARK MODEL

2008 ◽  
Vol 23 (27n30) ◽  
pp. 2413-2416 ◽  
Author(s):  
L. R. DAI ◽  
H. ZHANG ◽  
Y. FU ◽  
Z. Y. ZHANG ◽  
Y. W. YU
Keyword(s):  
Vector Meson ◽  
Quark Model ◽  
Short Range ◽  
Meson Exchange ◽  
Group Method ◽  
Short Range Interaction ◽  
Range Interaction ◽  
Baryon Interaction ◽  
The One ◽  
Vector Meson Exchange

The hyperon-nucleon scattering processes and some dibaryon states are studied both in the chiral SU(3) quark model and in the extended chiral SU(3) quark model by solving the resonating group method (RGM) equation. We find that the short-range interaction could be described either by the one-gluon exchange or by the vector meson exchange for baryon-baryon system.

scholarly journals THE SHORT RANGE MECHANISM OF N-N INTERACTION IN THE EXTENDED CHIRAL SU(3) QUARK MODEL

2005 ◽  
Vol 20 (08n09) ◽  
pp. 1994-1997 ◽  
Author(s):  
L. R. DAI ◽  
Z. Y. ZHANG ◽  
Y. W. YU
Keyword(s):  
Vector Meson ◽  
Quark Model ◽  
Short Range ◽  
Nucleon Nucleon ◽  
Phase Shifts ◽  
Short Range Interaction ◽  
Nucleon Interaction ◽  
Range Interaction ◽  
Nucleon Nucleon Interaction

We give the comparisons between the chiral SU (3) quark model and the extended chiral SU (3) quark model. The results show that the phase shifts of NN scattering are very similar. However, the short range mechanisms of nucleon-nucleon interaction are totally different. In the chiral SU (3) quark model, the short range interaction is dominantly from OGE, and in the extended chiral SU (3) quark model, it is dominantly from vector meson exchanges.

$\bar KN$ SCATTERING IN CHIRAL CONSTITUENT QUARK MODELS

2008 ◽  
Vol 23 (20) ◽  
pp. 3057-3072 ◽  
Author(s):  
F. HUANG ◽  
W. L. WANG ◽  
Z. Y. ZHANG
Keyword(s):  
Vector Meson ◽  
Quark Model ◽  
Cross Sections ◽  
Constituent Quark ◽  
Nucleon Nucleon ◽  
Phase Shifts ◽  
Meson Exchange ◽  
Group Method ◽  
Quark Interaction ◽  
Vector Meson Exchange

The chiral SU(3) quark model and the extended chiral SU(3) quark model have proven to be quite successful in reproducing the binding energy of the deuteron, the nucleon–nucleon (NN) scattering phase shifts and the hyperon–nucleon (YN) cross-sections. In the chiral SU(3) quark model, the quark–quark interaction contains one-gluon exchange (OGE), confinement potential and boson exchanges stemming from scalar and pseudoscalar nonets. In the extended chiral SU(3) quark model, the OGE is nearly replaced by vector meson exchange. It was shown in our previous work that these two models give quite similar descriptions for the S, P, D, F wave KN phase shifts, which means that in the KN system the contribution of OGE can be replaced by that of vector meson exchange. In this paper, we use the same models, the same parameters and the same methods to study the [Formula: see text] system with the purpose to test the effects of OGE and vector meson exchange. The cross-sections for K-p scattering into K-p, K0n, π+Σ-, π-Σ+, π0Σ0 and π0Λ channels are dynamically calculated by solving the resonating group method equation. While some channels are well described in one or the other model, a good agreement between the theoretical cross-sections and the experimental data for all channels is not successfully obtained. The present work indicates that both OGE and vector meson exchange are necessary to be included in the quark–quark interactions if one tries to simultaneously describe the KN phase shifts and [Formula: see text] cross-sections using one set of parameters in a constituent quark model.

scholarly journals Consistent Treatment of Pion Exchange Force and Meson versus Quark Dynamics in the Nucleon?Nucleon Interaction

1993 ◽  
Vol 46 (6) ◽  
pp. 737
Author(s):  
GQ Liu ◽  
AW Thomas
Keyword(s):  
Vector Meson ◽  
Short Range ◽  
Coupling Model ◽  
Nucleon Nucleon ◽  
Pion Exchange ◽  
Meson Exchange ◽  
Exchange Potential ◽  
Exchange Force ◽  
Gluon Exchange ◽  
Vector Meson Exchange

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.

scholarly journals Short range interaction in πJ/ψ − DD̄∗ channel

2019 ◽  
Vol 49 ◽  
pp. 1960005
Author(s):  
Yasuhiro Yamaguchi
Keyword(s):  
Lattice Qcd ◽  
Nuclear Physics ◽  
Short Range ◽  
Exchange Model ◽  
Meson Exchange ◽  
Heavy Flavor ◽  
Short Range Interaction ◽  
Range Interaction ◽  
Hadron Interaction ◽  
Exotic Hadrons

Exotic hadrons reported in the heavy flavor sector have attracted much interest in hadron and nuclear physics. Especially near the thresholds, the hadron-hadron interaction is important to understand these exotic structures. In this talk, the short range [Formula: see text] potential whose importance is indicated by the Lattice QCD is studied by the [Formula: see text] meson exchange model, and the Born-order quark exchange model. We find the large difference between the results of the [Formula: see text] meson exchange and the quark exchange calculations.

scholarly journals THE PENTAQUARKS IN THE LINEAR MOLECULAR HEPTAQUARK MODEL

2005 ◽  
Vol 20 (19) ◽  
pp. 4593-4598
Author(s):  
P. Bicudo
Keyword(s):  
Quark Model ◽  
Decay Width ◽  
Ground State ◽  
Short Range ◽  
Molecular System ◽  
Short Range Interaction ◽  
Range Interaction

In this talk, multiquarks are studied microscopically in a standard quark model. In pure ground-state pentaquarks the short-range interaction is computed and it is shown to be repulsive. An additional quark-antiquark pair is then considered, and this is suggested to produce linear molecular system, with a narrow decay width. The quarks assemble in three hadronic clusters, and the central hadron provides stability. The possible crypto-heptaquark hadrons with exotic pentaquark flavours, with strange, charmed and bottomed quarks, are predicted.

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