Abstract

The chiral constituent quark model (\(\chi \)CQM) is able to phenomenologically estimate the quantities having implications for chiral symmetry breaking and SU(3) symmetry breaking. In particular, it provides a fairly good description of the singlet (\(g^0_{A}\)) and non-singlet (\(g^3_{A}\) and \(g^8_{A}\)) axial-vector coupling constants at zero momentum transfer for the low lying octet baryons (N, \(\varSigma \), \(\varXi \) and \(\varLambda \)). We have used the conventional dipole form of parametrization to analyse the \(Q^2\) dependence of the axial-vector form factors (\(G^0_{A}(Q^2)\), \(G^3_{A}(Q^2)\) and \(G^8_{A}(Q^2)\)).

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.