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...
Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component...
We apply the discrete S_3 flavor symmetry to both lepton and quark sectors of the standard model ext...
AbstractThe S3 symmetry is shown to be a very good approximate symmetry when it is broken in a speci...
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...
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 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...
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...
Extent: 14p.By considering a flavour expansion about the SU(3)-flavour symmetric point, we investiga...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component...
We apply the discrete S_3 flavor symmetry to both lepton and quark sectors of the standard model ext...
AbstractThe S3 symmetry is shown to be a very good approximate symmetry when it is broken in a speci...
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...
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 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...
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...
Extent: 14p.By considering a flavour expansion about the SU(3)-flavour symmetric point, we investiga...
Using an SU(3) flavor symmetry breaking expansion in the quark mass, we determine the QCD component ...
Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component...
We apply the discrete S_3 flavor symmetry to both lepton and quark sectors of the standard model ext...
AbstractThe S3 symmetry is shown to be a very good approximate symmetry when it is broken in a speci...