Quark-antiquark states of the lightest scalar mesons within the Nambu-Jona-Lasinio model with flavor-dependent coupling constants
نویسندگان
چکیده
Abstract The quark-antiquark components of the U(3) lightest scalar meson nonet are investigated by considering Nambu-Jona-Lasinio model with flavor-dependent coupling constants that were derived (non-perturbative) gluon exchange. strange quark effective mass ($M_s^*$) is varied such strangeness content these mesons can be analyzed further. neutral states $S_0$, $S_8$ and $S_3$, adopted as most relevant respectively $\sigma(500)$, $f_0(980)$ $A_0^0(980)$ mesons. As a result, hierarchy between $S_0$ $S_8$, $K^*_0(700) - A_0(980)$ mesons, inverted corrected for quite low values constituent mass. Besides that, some particular $M_s^*$, masses $\sigma(500)$ also obtained mixing constant $G_{08}$. However, all nine not described simultaneously in self-consistent procedure, this goes along need non-quark-antiquark to completely describe their masses. A neutral-meson matrix defined leading angle found fitting correct value $\sigma (500) -f_0 (980)$ difference. Two different estimates strengths mixings $A_0^0 \to f_0$ $f_0 A_0^0$ proposed, somewhat behaviors. Firstly, assuming transitions intermediary flavor eigenstates secondly dynamical evolution. Results may good agreement experimental from BESS-III depending on
منابع مشابه
Metastable quark–antiquark droplets within the Nambu–Jona-Lasinio model
Chemically non–equilibrated quark–antiquark matter is studied within the Nambu–Jona-Lasinio model. The equations of state of non–strange (q = u, d) and strange (q = s) qq systems are calculated in the mean–field approximation. The existence of metastable bound states with zero pressure is predicted at finite densities and temperatures T ∼ 50 MeV. It is shown that the minimum energy per particle...
متن کاملStrange quark stars within the Nambu–Jona-Lasinio model
We investigate the properties of charge–neutral β–equilibrium cold quark matter within the Nambu–Jona-Lasinio model. The calculations are carried out for different ratios of coupling constants characterizing the vector and scalar 4–fermion interaction, ξ ≡ GV /GS . It is shown that for ξ < 0.4 matter is self–bound and for ξ < 0.65 it has a first order phase transition of the liquid– gas type. T...
متن کاملThe heavy mesons in Nambu–Jona-Lasinio model
We propose an extended Nambu–Jona-Lasinio model to include the heavy mesons with the heavy quark symmetry. The quark current-current interaction is generalized to include the heavy quark currents. In order to comply with the heavy quark spin symmetry at the heavy quark limit, the quark mass dependence of the interaction strength is introduced. The light and heavy pseudo-scalar and vector meson,...
متن کاملScalar mesons in the Nambu–Jona-Lasinio model with ’t Hooft interaction
We calculate the mass spectrum of the scalar meson nonet in the Nambu–JonaLasinio model (NJL model) with the ’t Hooft interaction. We also include corrections connected with meson loops in our analysis. The masses of the pseudoscalar and scalar meson nonets are in a satisfactory agreement with experimental data except for the mass of the f0(980) scalar meson. In order to describe this mass more...
متن کاملHeavy quark solitons in the Nambu-Jona-Lasinio model.
The Nambu–Jona-Lasinio model (NJL) is extended to incorporate heavy quark spinsymmetry. In this model baryons containing one heavy quark are analyzed as bound-states of light baryons, represented as chiral solitons, and mesons containing one heavy quark. From related studies in Skyrme type models, the ground-state heavy baryon is known to arise for the heavy meson in a P–wave configuration. In ...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
ژورنال
عنوان ژورنال: Journal of Physics G
سال: 2023
ISSN: ['1361-6471', '0954-3899']
DOI: https://doi.org/10.1088/1361-6471/acdaea