One of the more attractive aspects of the octet model(1) or “eightfold way” has been its ability to accommodate the N*, Y1*, and ≡* resonance in one isostrangeness multiplet, the (30)2. The (30) representation of SU3 is ten-dimensional as shown in Fig. 1. For this representation, the Okubo unitary mass formula(2,3) m=m0{1+aY+b[T(T+1)-1/4Y2]} (1) reduces to m=m0’(1+a’Y). (2
The system of strongly interacting particles is discussed, with electromagnetism, weak interactions,...
We study the interaction of vector mesons with the octet of stable baryons in the framework of the l...
We extend the recently developed treatment of baryon resonances in large N_c QCD to describe resonan...
In the framework of the octet model of unitary symmetry, we study in more detail the prediction of t...
We calculate the md-mu contribution to the mass splittings in baryonic isospin multiplets using SU(3...
The possibility that the ΔD35(1925) resonance is evidence for a [56, 1−] multiplet corresponding to ...
The Y0*(1405) resonance state is considered in terms of a multichannel potential arising from vector...
We calculate the md−mu contribution to the mass splittings in baryonic isospin multiplets using SU(3...
The investigation of the levels of the resonances which were recently discovered, is made by introdu...
The quantum group $ SU_{q}(3) = U_{q}(su(3))$ is taken as a baryon flavor symmetry. Accounting for e...
AbstractWe study the quark mass dependence of JP=1/2− s-wave baryon resonances. Parameter free resul...
The possibility that the D35(1925) resonance is evidence for a [56, 1-] multiplet corresponding to e...
The production of the octet of baryons and mesons in e+e- collisions is analyzed, based on considera...
Recently it has become apparent that many violations of SU(3) follow an octet pattern. For example, ...
The existence of a reciprocal bootstrap between baryon resonance decuplet with J=3/2± and baryon oct...
The system of strongly interacting particles is discussed, with electromagnetism, weak interactions,...
We study the interaction of vector mesons with the octet of stable baryons in the framework of the l...
We extend the recently developed treatment of baryon resonances in large N_c QCD to describe resonan...
In the framework of the octet model of unitary symmetry, we study in more detail the prediction of t...
We calculate the md-mu contribution to the mass splittings in baryonic isospin multiplets using SU(3...
The possibility that the ΔD35(1925) resonance is evidence for a [56, 1−] multiplet corresponding to ...
The Y0*(1405) resonance state is considered in terms of a multichannel potential arising from vector...
We calculate the md−mu contribution to the mass splittings in baryonic isospin multiplets using SU(3...
The investigation of the levels of the resonances which were recently discovered, is made by introdu...
The quantum group $ SU_{q}(3) = U_{q}(su(3))$ is taken as a baryon flavor symmetry. Accounting for e...
AbstractWe study the quark mass dependence of JP=1/2− s-wave baryon resonances. Parameter free resul...
The possibility that the D35(1925) resonance is evidence for a [56, 1-] multiplet corresponding to e...
The production of the octet of baryons and mesons in e+e- collisions is analyzed, based on considera...
Recently it has become apparent that many violations of SU(3) follow an octet pattern. For example, ...
The existence of a reciprocal bootstrap between baryon resonance decuplet with J=3/2± and baryon oct...
The system of strongly interacting particles is discussed, with electromagnetism, weak interactions,...
We study the interaction of vector mesons with the octet of stable baryons in the framework of the l...
We extend the recently developed treatment of baryon resonances in large N_c QCD to describe resonan...