The value of the nucleon's flavour-singlet axial-charge extracted from polarised deep inelastic scattering is sensitive to the value of the octet axial-charge gA(8) which is usually taken from an analysis of hyperon β-decays within the framework of SU(3) symmetry, namely 0.58 ± 0.03. Using the Cloudy Bag model we find that the value of gA(8) is reduced by as much as 20% below the usual phenomenological value. This increases the value of the flavour-singlet axial-charge (gA(0) |inv) derived from deep inelastic data and significantly reduces the difference between it and gA(8). © 2010 Elsevier B.V. All rights reserved.Steven D. Bass and Anthony W. Thoma
The axial charge of the nucleon gA and the pion decay constant fπ are computed in two-flavor lattice...
With the chiral quark model, we have calculated the axial charges of the pentaquark states with (I, ...
AbstractIn chiral models with SU(3) group structure, strange form factors of baryon octet are evalua...
AbstractThe value of the nucleon's flavour-singlet axial-charge extracted from polarised deep inelas...
The nucleon's axial charge, gA, expresses features that are both fundamental to the strong interacti...
We report on our calculation of the nucleon axial charge gA in QCD with two flavours of dynamical qu...
The nucleon self-energy and its relation to the nucleon axial charge gA are discussed at large Nc. T...
The light-quark mass dependence of the nucleon axial isovector charge (gA) has been studied up to ne...
The octet-baryon axial-vector charges and the g(1)/f(1) ratios measured in the semileptonic hyperon ...
We have investigated the axial charges of the nucleon and N* resonances in a...
The theory of the `proton spin' effect proposed in our earlier papers is extended to include the chi...
AbstractThe axial charge of the nucleon gA and the pion decay constant fπ are computed in two-flavor...
The axial coupling of the nucleon, gA, is the strength of its coupling to the weak axial current of ...
We present recent Monte Carlo data for the axial charge of the nucleon obtained by the QCDSF-UKQCD c...
The axial coupling of the nucleon, gA, is the strength of its coupling to the weak axial current of ...
The axial charge of the nucleon gA and the pion decay constant fπ are computed in two-flavor lattice...
With the chiral quark model, we have calculated the axial charges of the pentaquark states with (I, ...
AbstractIn chiral models with SU(3) group structure, strange form factors of baryon octet are evalua...
AbstractThe value of the nucleon's flavour-singlet axial-charge extracted from polarised deep inelas...
The nucleon's axial charge, gA, expresses features that are both fundamental to the strong interacti...
We report on our calculation of the nucleon axial charge gA in QCD with two flavours of dynamical qu...
The nucleon self-energy and its relation to the nucleon axial charge gA are discussed at large Nc. T...
The light-quark mass dependence of the nucleon axial isovector charge (gA) has been studied up to ne...
The octet-baryon axial-vector charges and the g(1)/f(1) ratios measured in the semileptonic hyperon ...
We have investigated the axial charges of the nucleon and N* resonances in a...
The theory of the `proton spin' effect proposed in our earlier papers is extended to include the chi...
AbstractThe axial charge of the nucleon gA and the pion decay constant fπ are computed in two-flavor...
The axial coupling of the nucleon, gA, is the strength of its coupling to the weak axial current of ...
We present recent Monte Carlo data for the axial charge of the nucleon obtained by the QCDSF-UKQCD c...
The axial coupling of the nucleon, gA, is the strength of its coupling to the weak axial current of ...
The axial charge of the nucleon gA and the pion decay constant fπ are computed in two-flavor lattice...
With the chiral quark model, we have calculated the axial charges of the pentaquark states with (I, ...
AbstractIn chiral models with SU(3) group structure, strange form factors of baryon octet are evalua...