Chiral SU(3) Quack Model and Multiquark State. Zhang Zong ye (Institute of High Energy Physics, Beijing). Outline. Introduction Chiral SU(3) Quark Model and NN , YN and KN scatterings Dibaryon Pentaquark state. Introduction.
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Zhang Zong ye
(Institute of High Energy Physics, Beijing)
and NN , YN and KN scatterings
The NPQCD effect is very important for the light quark system.But up to now, there is no effective approach to solve the NPQCD problem seriously. We still need QCD inspired model to help.
In theframework of the constituent quark model, to understand
the source of the constituent quark mass, the spontaneous vacuum breaking has to be considered, and as a consequence, the coupling between quark field and goldstone boson is introduced to restore the chiral symmetry.
The chiral quark model can be regarded as a quite reasonable and useful model to describe the medium range NPQCD effect.
First we generalized the chiral SU(2) quark model to chiral
SU(3) quark model for studying the system withsquark and try to
see if we can get a unified explanation of N-N and Y-N data on
Then we extend the study to the multiquark system..
Since for the multiquark states, quarks should stay in a small area,
the quark exchange effect must be important. We didan analysis to
see the quark exchange effect in two baryon systems. We found
that: the quark exchange effect of some cases is not important; some
cases have very strong Pauli Block Effect, and for some cases it makes
these two baryon cluster close together--- it is favorable to make two
baryon to be bound.
According to the analysis, using chiral SU(3) quark model with the
same parameters we used in the scattering calculations, we got :
A new interesting dibaryon candidate - - - di-Omega .
We also studiedthe structure of the pentaquark state .
In the chiral SU(3) quark model, the coupling between chiral field
and quark is introducedto describe low momentum medium range
NPQCD effect.The interacting Lagrangian can be written as:
scalar nonet fields pseudo-scalar nonet fields
It is easy to prove that is invariant under the infinitesimal chiral
transformation. This can be regarded asan extension of the SU(2) - σ model for
studying the system with s quark.
interaction to govern the short range behavior, and a confinement
potential to provide the NPQCD effect in the long distance.
Hamiltonian of the system:
( is taken as quadratic form.)
Here we have only one coupling constant,
(1). Input part: taken to be the usual values.
(2). Chiral field part:
( are taken to be experimental values, )
(3). OGE and confinement part:
and are fixed by and .
are determined by the stability condition of
N-N,Y-N K-N OGE
0 35.3 (-18)
48.1 52.4 (55.2)
Expt. Theor. Expt. Theor.
N939 939 Δ 1232 1237
Λ 1116 1116 1385 1375
Σ 1193 1194 1530 1515
Ξ 1319 1334 1672 1657
To study the two baryon system, we did a two-cluster dynamical RGM calculation
Phase shifts of N-N scattering
Y-N dynamical RGM calculation cross sections of
Y-N cross sections of dynamical RGM calculation
Phase shifts of K-N scattering dynamical RGM calculation
K-N D wave dynamical RGM calculation
K-N F wave dynamical RGM calculation
When dynamical RGM calculation the quark exchange effect
is not important,
the Pauli Block Effect
is very serious,
the quark exchange effect
makes two baryon cluster closer.
It has so-called quantum
In all of two baryon systems, only 6 of them belong to this interesting case,
Only has enough long lifetime, because it can’t decay through
State dynamical RGM calculation B(MeV)
H partical ~ 2 (near 2Λ threshold)
The results are calculated by using chiral SU(3) quark model with the same parameters we used in the NN and YN scattering processes.
State dynamical RGM calculation B(MeV)
is the most interesting one, because it
can’t decay through strong interactions , and thus
it has enough long lifetime.
Main properties of dynamical RGM calculation :
1). Binding energy several tens to hundred MeV,
2). Distance between two , 0.8fm,
3). It carries –2 charges,
4). Mean lifetime sec.
All of them are weak decays.
How the result dependent on the parameters is. dynamical RGM calculation
Fit NN Fit KN
137.4 61.2 134.4
Even the mixing of and is taken to be ideally mixing, i.e. there is no
meson exchange between two s quarks, the binding energy of is
still quite large , around 60 MeV. This result tells us again thatthe symmetry
property of is really very important to make it bound.
is a very interesting new dibaryon candidate, dynamical RGM calculation
but how to search it seems not so easy, because its
production rate is rare.
Some authors estimated its production rate in the relativistic heavy ion
collision processes at RHIC energy by using different models.
Their results show: the ratio of the production rate of
and single ,
Though the searching work is hard, RHIC-STAR group still plans to try to
search it in the heavy ion collision processes and has listed this work in
their research proposal.
4 configurations of and 4 of are considered. They are:
5q states with different size b :
and solve to get
Results tell us that:
It seems that quark model.in the framework of the chiral SU(3) quark model,
when the parameters are taken in the reasonable region, it is difficult to get the mass of Θ to be closed to the experimental value (1540 MeV).
Summary: quark model.