AbstractWe study the quark mass dependence of JP=1/2− s-wave baryon resonances. Parameter free results are obtained in terms of the leading order chiral Lagrangian. In the ‘heavy’ SU(3) limit with mπ=mK≃500 MeV the resonances turn into bound states forming two octets plus a singlet representations of the SU(3) group. A contrasted result is obtained in the ‘light’ SU(3) limit with mπ=mK≃140 MeV for which no resonances exist. Using physical quark masses our analysis suggests to assign to the S=−2 resonances Ξ(1690) and Ξ(1620) the quantum numbers JP=1/2−
The s-wave meson-baryon interaction in the S = -1, S = 0 and S = -2 sectors is studied by means of c...
We argue that three-quark excited states naturally group into quartets, split into two parity double...
We argue that three-quark excited states naturally group into quartets, split into two parity double...
We study the quark mass dependence of J(P) = 1/2(-) s-wave baryon resonances. Parameter free results...
We study the quark mass dependence of J(P) = 1/2(-) s-wave baryon resonances. Parameter free results...
We study the quark-mass dependence of J(P) = (1/2-) s-wave and J(P) = 3/2(-) d-wave baryon resonance...
We study the quark mass dependence of $J^P = \frac12^-$ s-wave baryon resonances. Parameter free res...
The s-wave meson-baryon interaction in the S=−1 sector is studied by means of coupled-channels, usin...
Using the lowest order chiral Lagrangian we study s-wave interactions of the baryon decuplet with th...
We argue that selected S wave meson-baryon channels may play a key role in matching poor baryon mass...
Using a unitary extension of chiral perturbation theory with a lowest-order s-wave SU(3) chiral Lagr...
We study S-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons using the ...
The mechanism for the formation of the $\Lambda(1405)$ resonance is studied in a chiral quark model ...
We study $J^P=({3/2})^-$ baryon resonances as generated by chiral coupled-channel dynamics. Paramete...
The s-wave meson-baryon interaction in the S = -1, S = 0 and S = -2 sectors is studied by means of c...
The s-wave meson-baryon interaction in the S = -1, S = 0 and S = -2 sectors is studied by means of c...
We argue that three-quark excited states naturally group into quartets, split into two parity double...
We argue that three-quark excited states naturally group into quartets, split into two parity double...
We study the quark mass dependence of J(P) = 1/2(-) s-wave baryon resonances. Parameter free results...
We study the quark mass dependence of J(P) = 1/2(-) s-wave baryon resonances. Parameter free results...
We study the quark-mass dependence of J(P) = (1/2-) s-wave and J(P) = 3/2(-) d-wave baryon resonance...
We study the quark mass dependence of $J^P = \frac12^-$ s-wave baryon resonances. Parameter free res...
The s-wave meson-baryon interaction in the S=−1 sector is studied by means of coupled-channels, usin...
Using the lowest order chiral Lagrangian we study s-wave interactions of the baryon decuplet with th...
We argue that selected S wave meson-baryon channels may play a key role in matching poor baryon mass...
Using a unitary extension of chiral perturbation theory with a lowest-order s-wave SU(3) chiral Lagr...
We study S-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons using the ...
The mechanism for the formation of the $\Lambda(1405)$ resonance is studied in a chiral quark model ...
We study $J^P=({3/2})^-$ baryon resonances as generated by chiral coupled-channel dynamics. Paramete...
The s-wave meson-baryon interaction in the S = -1, S = 0 and S = -2 sectors is studied by means of c...
The s-wave meson-baryon interaction in the S = -1, S = 0 and S = -2 sectors is studied by means of c...
We argue that three-quark excited states naturally group into quartets, split into two parity double...
We argue that three-quark excited states naturally group into quartets, split into two parity double...