The Quadratic mass formula in the quartet model is applied to vector- and pseudoscalar-mesons in order to determine their quark contents. A mixing scheme of all the three iso-singlet states, φ_0, φ_8 and φ_<15>, is proposed, which leads to a reasonable value of small hadronic decay width of J/ψ
Our previous calculations of the sea- and valence-quark mass dependence of the pseudoscalar meson ma...
In order to get a more realistic description of the hadron spectrum we extend a constituent-quark mo...
Our previous calculations of the sea- and valence-quark mass dependence of the pseudoscalar meson ma...
The possibility that ¢-particles are vector-mesons composed of a charmed quark and an anti-charmed q...
The mass splittings within the SU(2) multiplets of pseudoscalar mesons (π, K, D, B) are used as a la...
The fourth Standard Model (SM) family quarks and weak iso-singlet quarks predicted by E-6 GUT are co...
We present an SU(3)(F) meson mass formula from random phase approximation. Both the mesons of ground...
The axial-vector Ward-Takahashi identity is used to derive mass formulas for neutral pseudoscalar me...
We show that a linear scaling between the weak decay constants of pseudoscalars and the vector meson...
By comparing SU(3)-breaking scales of linear mass formulae, it is shown that the lowest vector, axia...
We show that a linear scaling between the weak decay constants of pseudoscalars and the vector meson...
In order to get a more realistic description of the hadron spectrum we extend a constituentquark mod...
The spectroscopic parameters and partial decay widths of the light mesons a0(980) and K0⁎(800) are c...
A differential equation for meson states is derived from the Bethe-Salpeter equation under the cond...
Gupta V, Kögerler R. Predictions for the meson masses in broken flavour SU(5) symmetry. REVISTA MEXI...
Our previous calculations of the sea- and valence-quark mass dependence of the pseudoscalar meson ma...
In order to get a more realistic description of the hadron spectrum we extend a constituent-quark mo...
Our previous calculations of the sea- and valence-quark mass dependence of the pseudoscalar meson ma...
The possibility that ¢-particles are vector-mesons composed of a charmed quark and an anti-charmed q...
The mass splittings within the SU(2) multiplets of pseudoscalar mesons (π, K, D, B) are used as a la...
The fourth Standard Model (SM) family quarks and weak iso-singlet quarks predicted by E-6 GUT are co...
We present an SU(3)(F) meson mass formula from random phase approximation. Both the mesons of ground...
The axial-vector Ward-Takahashi identity is used to derive mass formulas for neutral pseudoscalar me...
We show that a linear scaling between the weak decay constants of pseudoscalars and the vector meson...
By comparing SU(3)-breaking scales of linear mass formulae, it is shown that the lowest vector, axia...
We show that a linear scaling between the weak decay constants of pseudoscalars and the vector meson...
In order to get a more realistic description of the hadron spectrum we extend a constituentquark mod...
The spectroscopic parameters and partial decay widths of the light mesons a0(980) and K0⁎(800) are c...
A differential equation for meson states is derived from the Bethe-Salpeter equation under the cond...
Gupta V, Kögerler R. Predictions for the meson masses in broken flavour SU(5) symmetry. REVISTA MEXI...
Our previous calculations of the sea- and valence-quark mass dependence of the pseudoscalar meson ma...
In order to get a more realistic description of the hadron spectrum we extend a constituent-quark mo...
Our previous calculations of the sea- and valence-quark mass dependence of the pseudoscalar meson ma...
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