The decay rates of baryon resonances assigned to the (70, 1/sup -/) and (56, 2/sup +/) representations of SU(6)/sub w/(X)O(3) are subjected to a detailed comparison with an SU(6)/sub w/ model motivated by the work of Melosh (see abstr. A59579 of 1974). SU(6)/sub w/ is remarkably successful as an approximate symmetry for decay vertices. (44 refs)
A consistent SU(6) extension of the Weinberg-Tomozawa meson-baryon chiral Lagrangian is constructed ...
The phases of resonant amplitudes in pi N to pi Delta are studied in a modified version of SU(6)/sub...
The phenomenological prescriptions outlined in the preceding paper (I) for meson-baryon couplings in...
The author discusses the decays of baryon resonances, classified in the (70,1/sup -/) and (56,2/sup ...
The authors present a least squares fit to the experimental data on decays of negative parity baryon...
An SU(6)×O(3) model of baryons, which had earlier been used by Mitra and Ross for the evaluatio...
The transformation between ''current'' quarks and ''constituent'' quarks recently suggested by Melos...
A new form of parametrization is proposed for meson-baryon couplings in a phenomenological quark (Q)...
The possibility of some natural odd parity Δ states in the latest PDG tables belonging to (56, ...
The excitation function for the 0h/2 pi omega and 1h/2 pi omega levels of /sub Lambda //sup 6/Li, po...
Constituent quark models provide a reasonable description of the baryon mass spectra. However, even ...
The positive- and negative-parity baryon mass shifts are investigated under the assumption that thes...
Evidence for the existence of exotic, pentaquark baryons was first found in the invariant mass spect...
Vector meson degrees of freedom are incorporated into the Weinberg-Tomozawa (WT) meson-baryon chiral...
In the colored-quark model, if the three vector gluons that correspond to an SU(2) subgroup of SU(3)...
A consistent SU(6) extension of the Weinberg-Tomozawa meson-baryon chiral Lagrangian is constructed ...
The phases of resonant amplitudes in pi N to pi Delta are studied in a modified version of SU(6)/sub...
The phenomenological prescriptions outlined in the preceding paper (I) for meson-baryon couplings in...
The author discusses the decays of baryon resonances, classified in the (70,1/sup -/) and (56,2/sup ...
The authors present a least squares fit to the experimental data on decays of negative parity baryon...
An SU(6)×O(3) model of baryons, which had earlier been used by Mitra and Ross for the evaluatio...
The transformation between ''current'' quarks and ''constituent'' quarks recently suggested by Melos...
A new form of parametrization is proposed for meson-baryon couplings in a phenomenological quark (Q)...
The possibility of some natural odd parity Δ states in the latest PDG tables belonging to (56, ...
The excitation function for the 0h/2 pi omega and 1h/2 pi omega levels of /sub Lambda //sup 6/Li, po...
Constituent quark models provide a reasonable description of the baryon mass spectra. However, even ...
The positive- and negative-parity baryon mass shifts are investigated under the assumption that thes...
Evidence for the existence of exotic, pentaquark baryons was first found in the invariant mass spect...
Vector meson degrees of freedom are incorporated into the Weinberg-Tomozawa (WT) meson-baryon chiral...
In the colored-quark model, if the three vector gluons that correspond to an SU(2) subgroup of SU(3)...
A consistent SU(6) extension of the Weinberg-Tomozawa meson-baryon chiral Lagrangian is constructed ...
The phases of resonant amplitudes in pi N to pi Delta are studied in a modified version of SU(6)/sub...
The phenomenological prescriptions outlined in the preceding paper (I) for meson-baryon couplings in...
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