Add to ORKGBy considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavour-blindness constrains octet baryon matrix elements after SU(3) is broken by the mass difference between the strange and light quarks. We find the expansions to be highly constrained along a mass trajectory where the singlet quark mass is held constant, which proves beneficial for extrapolations of 2+1 flavour lattice data to the physical point. We investigate these effects numerically via a lattice calculation of the flavour-conserving and flavour-changing matrix elements of the vector and axial operators between octet baryon states
Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component...
QCD lattice simulations with 2+1 flavours (when two quark flavours are mass degenerate) typically st...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
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...
Extent: 14p.By considering a flavour expansion about the SU(3)-flavour symmetric point, we investiga...
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 ...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
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 S U ( 3 ) flavor symmetric point, we investigate how fla...
Using an SU(3) flavour 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...
QCD lattice simulations with 2+1 flavours (when two quark flavours are mass degenerate) typically st...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...
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...
Extent: 14p.By considering a flavour expansion about the SU(3)-flavour symmetric point, we investiga...
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 ...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
By considering a flavor expansion about the SU(3) flavor symmetric point, we investigate how flavor ...
Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we de...
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 S U ( 3 ) flavor symmetric point, we investigate how fla...
Using an SU(3) flavour 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...
QCD lattice simulations with 2+1 flavours (when two quark flavours are mass degenerate) typically st...
The SU(3) flavour symmetry breaking expansion in up, down and strange quark masses is extended from ...