The quantum group $ SU_{q}(3) = U_{q}(su(3))$ is taken as a baryon flavor symmetry. Accounting for electromagnetic contributions to baryons masses up to zeroth order, new charge specific q-deformed octet and decuplet baryon mass formulas are obtained. These new mass relations have errors of only 0.02% and 0.08%, respectively, a factor of 20 reduction compared to the standard Gell-Mann-Okubo mass formulas. A new relation between the octet and decuplet baryon masses that is accurate to 1.2% is derived. An explicit formula for the Cabibbo angle, taken to be $\frac{\pi}{14}$, in terms of the deformation parameter q and spin parity JP of the baryons is obtained
Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
By comparing SU(3)-breaking scales of linear mass formulae, it is shown that the lowest vector, axia...
Using instead of ordinary flavour symmetries SU(n_f) their corresponding quantum (q-deformed) analog...
The effects of symmetry breaking and renormalization on a unified field theory can be simulated by t...
We investigate the electromagnetic form factors of the baryon decuplet within the framework of the $...
Baryon masses of the flavour SU(3) octet and decuplet baryons are calculated in the framework of the...
Baryon masses and nucleon σ terms are studied with the effective theory that combines the chiral and...
Baryon masses of the flavour SU(3) octet and decuplet baryons are calculated in the framework of the...
The electromagnetic form factors of octet baryons are investigated from the stand-point that the bar...
I discuss the quark mass dependence of various baryon properties derived from chiral perturbation th...
The positive- and negative-parity baryon mass shifts are investigated under the assumption that thes...
Copyright © 2002 Published by Elsevier Science B.V. All rights reserved.A new intuitive method for t...
I discuss the quark mass dependence of various baryon properties derived from chiral perturbation th...
1/N[subscript c] baryon mass relations are compared with lattice simulations of baryon masses using ...
Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
By comparing SU(3)-breaking scales of linear mass formulae, it is shown that the lowest vector, axia...
Using instead of ordinary flavour symmetries SU(n_f) their corresponding quantum (q-deformed) analog...
The effects of symmetry breaking and renormalization on a unified field theory can be simulated by t...
We investigate the electromagnetic form factors of the baryon decuplet within the framework of the $...
Baryon masses of the flavour SU(3) octet and decuplet baryons are calculated in the framework of the...
Baryon masses and nucleon σ terms are studied with the effective theory that combines the chiral and...
Baryon masses of the flavour SU(3) octet and decuplet baryons are calculated in the framework of the...
The electromagnetic form factors of octet baryons are investigated from the stand-point that the bar...
I discuss the quark mass dependence of various baryon properties derived from chiral perturbation th...
The positive- and negative-parity baryon mass shifts are investigated under the assumption that thes...
Copyright © 2002 Published by Elsevier Science B.V. All rights reserved.A new intuitive method for t...
I discuss the quark mass dependence of various baryon properties derived from chiral perturbation th...
1/N[subscript c] baryon mass relations are compared with lattice simulations of baryon masses using ...
Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
By comparing SU(3)-breaking scales of linear mass formulae, it is shown that the lowest vector, axia...