By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor blindness constrains octet baryon matrix elements after SU(3) is broken by the mass difference between quarks. Similarly to hadron masses we find the expansions to be constrained along a mass trajectory where the singlet quark mass is held constant, which provides invaluable insight into the mechanism of flavor symmetry breaking and proves beneficial for extrapolations to the physical point. Expansions are given up to third order in the expansion parameters. Considering higher orders would give no further constraints on the expansion parameters. The relation of the expansion coefficients to the quark-line-connected and quark-line-disconnected...
QCD lattice simulations with 2+1 flavors (when two quark flavors are mass degenerate) typically star...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
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 ...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavo...
Extent: 14p.By considering a flavour expansion about the SU(3)-flavour symmetric point, we investiga...
By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavo...
By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavo...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
QCD lattice simulations with 2+1 flavors (when two quark flavors are mass degenerate) typically star...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
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 ...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavo...
Extent: 14p.By considering a flavour expansion about the SU(3)-flavour symmetric point, we investiga...
By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavo...
By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavo...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
QCD lattice simulations with 2+1 flavors (when two quark flavors are mass degenerate) typically star...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...