We evaluate the pseudoscalar-meson octet-baryon coupling constants and the corresponding axial charges in eight channels (πNN, πΣΣ, πΛΣ, KΛN, KΣN, πΞΞ, KΛΞ and KΣΞ) in lattice QCD with two flavors of dynamical quarks. The parameter α≡F/(F+D) representing the SU(3)-flavor symmetry is computed at each u,d-quark hopping parameter and at the flavor-SU(3) symmetric point where the three quark flavors are degenerate at the physical s-quark mass. In particular, we obtain α=0.395(6) at the SU(3) symmetric limit. The quark-mass dependences of the coupling constants are obtained by changing the u- and the d-quark masses and we find that the SU(3)-flavor symmetry is broken by only a few percent at each quark-mass we employ.pre-prin
Lattice QCD affords us the unique opportunity to study the quark structure of hadrons non-perturbati...
We evaluate the strangeness-conserving NN, ΣΣ, ΞΞ, ΛΣ and the strangeness-changing ΛN, ΣN, ΛΞ, ΣΞ a...
We determine the axial, scalar and tensor isovector charges of the nucleon, sigma and cascade baryon...
We evaluate the pseudoscalar-meson coupling constants and the strangeness-conservingand the strangen...
Lattice QCD simulations are now reaching a precision where isospin breaking effects become important...
We present results for the ground-state mass shifts of octet baryons due to the presence of a medium...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
By considering a flavor expansion about the S U ( 3 ) flavor symmetric point, we investigate how fla...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
The spectra of octet and decuplet baryons are studied using SU(3) lattice QCD at the quenched level....
Lattice quantum chromodynamics is used to constrain the interactions of two octet baryons at the SU(...
National Science Foundation (U.S.) (PHY11-25915)United States. Department of Energy (DE-SC00-10495)U...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
We investigate the strong coupling constants for the baryon octet–octet, decuplet–octet, and decuple...
In the Standard Model of particle physics quarks and gluons are bound by the fundamental strong forc...
Lattice QCD affords us the unique opportunity to study the quark structure of hadrons non-perturbati...
We evaluate the strangeness-conserving NN, ΣΣ, ΞΞ, ΛΣ and the strangeness-changing ΛN, ΣN, ΛΞ, ΣΞ a...
We determine the axial, scalar and tensor isovector charges of the nucleon, sigma and cascade baryon...
We evaluate the pseudoscalar-meson coupling constants and the strangeness-conservingand the strangen...
Lattice QCD simulations are now reaching a precision where isospin breaking effects become important...
We present results for the ground-state mass shifts of octet baryons due to the presence of a medium...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
By considering a flavor expansion about the S U ( 3 ) flavor symmetric point, we investigate how fla...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
The spectra of octet and decuplet baryons are studied using SU(3) lattice QCD at the quenched level....
Lattice quantum chromodynamics is used to constrain the interactions of two octet baryons at the SU(...
National Science Foundation (U.S.) (PHY11-25915)United States. Department of Energy (DE-SC00-10495)U...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
We investigate the strong coupling constants for the baryon octet–octet, decuplet–octet, and decuple...
In the Standard Model of particle physics quarks and gluons are bound by the fundamental strong forc...
Lattice QCD affords us the unique opportunity to study the quark structure of hadrons non-perturbati...
We evaluate the strangeness-conserving NN, ΣΣ, ΞΞ, ΛΣ and the strangeness-changing ΛN, ΣN, ΛΞ, ΣΞ a...
We determine the axial, scalar and tensor isovector charges of the nucleon, sigma and cascade baryon...