Bound states in the colored-quark model

1974 ◽  
Vol 49 (2) ◽  
pp. 178-180 ◽  
Author(s):  
R.H. Capps
Keyword(s):  
Quark Model ◽  
Bound States

scholarly journals The Genuine Resonance of Full-Charm Tetraquarks

Universe ◽  
2021 ◽  
Vol 7 (5) ◽  
pp. 155
Author(s):  
Xiaoyun Chen
Keyword(s):  
Quark Model ◽  
Bound States ◽  
Expansion Method ◽  
Chiral Quark Model ◽  
Stabilization Method ◽  
Scaling Method ◽  
Resonance States ◽  
Gaussian Expansion Method ◽  
Color Structure ◽  
Quantum Numbers

In this work, the genuine resonance states of full-charm tetraquark systems with quantum numbers JPC=0++,1+−,2++ are searched in a nonrelativistic chiral quark model with the help of the Gaussian Expansion Method. In this calculation, two structures, meson-meson and diquark–antidiquark, as well as their mixing with all possible color-spin configurations, are considered. The results show that no bound states can be formed. However, resonances are possible because of the color structure. The genuine resonances are identified by the stabilization method (real scaling method). Several resonances for the full-charm system are proposed, and some of them are reasonable candidates for the full-charm states recently reported by LHCb.

scholarly journals POSSIBLE $D\bar{D}$ AND $B\bar{B}$ MOLECULAR STATES IN A CHIRAL QUARK MODEL

2012 ◽  
Vol 27 (27) ◽  
pp. 1250161 ◽  
Author(s):  
M. T. LI ◽  
W. L. WANG ◽  
Y. B. DONG ◽  
Z. Y. ZHANG
Keyword(s):  
Quark Model ◽  
Systematic Study ◽  
Bound States ◽  
Effective Interaction ◽  
Bound State ◽  
Chiral Quark Model ◽  
State Problem ◽  
Bound State Problem

We perform a systematic study of the bound state problem of [Formula: see text] and [Formula: see text] systems by using effective interaction in our chiral quark model. Our results show that both the interactions of [Formula: see text] and [Formula: see text] states are attractive, which consequently result in [Formula: see text] and [Formula: see text] bound states.

scholarly journals Doubly charmed multibaryon systems

2020 ◽  
Vol 80 (8) ◽  
Author(s):  
H. Garcilazo ◽  
A. Valcarce
Keyword(s):  
Quark Model ◽  
Bound States ◽  
Constituent Quark ◽  
Constituent Quark Model ◽  
Heavy Quarks ◽  
Separation Energy ◽  
Quantum Numbers ◽  
Body State

Abstract We study two- and three-baryon systems with two units of charm looking for possible bound states or resonances. All two-baryon interactions are consistently derived from a constituent quark model tuned in the light-flavor hadron phenomenology: spectra and interactions. The presence of the heavy quarks makes the two-body interactions simpler than in the light-flavor sector. Our results show a narrow two-body resonance with quantum numbers $$(I,J^P)=(0,0^+)$$(I,JP)=(0,0+). It is located 6.2 MeV below the $$\Sigma _c\Sigma _c$$ΣcΣc threshold and has a width of 4.7 MeV. The foregoing two-body state contributes to generate a $$N \Sigma _c\Sigma _c$$NΣcΣc resonance with quantum numbers $$(I,J^P)=(1/2,1/2^+)$$(I,JP)=(1/2,1/2+) and a separation energy of 0.2 MeV.

Prediction of Double-heavy Tetraquarks Bound States in Quark Model

2021 ◽  
Vol 62 (4) ◽  
Author(s):  
Qi Meng ◽  
Emiko Hiyama ◽  
Atsushi Hosaka ◽  
Makoto Oka ◽  
Philipp Gubler ◽  
...  
Keyword(s):  
Quark Model ◽  
Bound States

The Quark Model

2019 ◽  
pp. 55-76
Author(s):  
Michael E. Peskin
Keyword(s):  
Quark Model ◽  
Bound States ◽  
B Quarks ◽  
S Quarks

This chapter presents the quark model of hadrons. It discusses the quark description of the quark antiquark systems of c and b quarks. It then describes the structure of the lightest mesons and baryons as bound states of u, d, and s quarks.

The possible strangeness dibaryon states in a chiral quark model

2015 ◽  
Vol 30 (09) ◽  
pp. 1550048
Author(s):  
L. R. Dai ◽  
L. Yuan ◽  
N. Zheng ◽  
X. S. Kang ◽  
S. L. Yuan ◽  
...  
Keyword(s):  
Quark Model ◽  
Bound States ◽  
Good Description ◽  
Nucleon Nucleon ◽  
Group Method ◽  
Model Parameters ◽  
Chiral Quark Model ◽  
Scalar Mesons ◽  
Ideal Mixing ◽  
The Ideal

Considering the mixing of scalar mesons, the ΩΩ and Ξ*Ω systems are dynamically investigated within the framework of the chiral SU(3) quark model by solving the resonating group method (RGM) equation. The model parameters are taken from our previous work, which gave a good description of the energies of the baryon ground states, the binding energy of deuteron, and the experimental data of the nucleon–nucleon (NN) and nucleon–hyperon (NY) scattering processes. Two different mixing cases, one is the ideal mixing and another is 19° mixing, are discussed. The results show that no matter what kind of mixing is adopted, the ΩΩ and Ξ*Ω systems are still bound states. It is also shown that they are deeply bound if 19° mixing is adopted.

scholarly journals Masses of Charmed and Bottom Tetraquarks in the Non-Relativistic Quark Model

2018 ◽  
Vol 46 ◽  
pp. 1860084 ◽  
Author(s):  
Zahra Ghalenovi
Keyword(s):  
Wave Function ◽  
Quark Model ◽  
Bound States ◽  
Constituent Quark ◽  
Constituent Quark Model ◽  
Relativistic Quark Model ◽  
Scalar State ◽  
State Formula ◽  
The Masses ◽  
Scalar Resonances

Heavy tetraquark states are studied within the diquark-antidiquark picture in the framework of a simple constituent quark model. Considering hyperfine spin and isospin interactions, we predict the masses of the scalar diquarks and of the open and hidden charmed and bottom scalar tetraquarks. Our results indicate the scalar resonances [Formula: see text] and [Formula: see text] have a sizable tetraquark amount in their wave function, while it turns out the scalar state [Formula: see text] should not be considered as being predominately diquark-antidiquark bound states.

scholarly journals Relativistic Bound States

1991 ◽  
Vol 44 (3) ◽  
pp. 149 ◽  
Author(s):  
BHJ McKellar
Keyword(s):  
Quark Model ◽  
Uncertainty Principle ◽  
Light Cone ◽  
Bound States ◽  
Relativistic Effects ◽  
Relativistic Dynamics ◽  
Hadronic Structure ◽  
Quark Structure ◽  
Relativistic Bound States

The standard resul ts of the quark model rely on nonrelativistic descriptions of the wavefunctions of the quarks in the hadron. However, simple uncertainty principle considerations show that the momenta of the quarks are comparable to their (constituent) masses, so that relativistic dynamics must be used in the description of the hadronic structure. In this paper I describe a number of new and old results which illustrate relativistic effects on the quark structure of hardons, and which employ the method of light cone quantisation to handle relativity.

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