Harleen Dahiya

Octet and decuplet baryon magnetic moments in the chiral quark model

Octet and decuplet baryon magnetic moments have been formulated within the chiral quark model

Chiral quark model with configuration mixing

(ensuremath{chi}mathrm{QM})

Octet magnetic moments and the Coleman-Glashow sum rule violation in the chiral quark model

with configuration mixing incorporating the sea quark polarizations and their orbital angular momentum through a generalization of the Cheng-Li mechanism. When the parameters of the

SU(4) chiral quark model with configuration mixing

ensuremath{chi}mathrm{QM}

Parton Distributions in Impact Parameter Space

without configuration mixing are fixed by incorporating the latest data pertaining to

Chiral constituent quark model and the coupling strength of eta

ifmmode bar{u}else ={u}fi{}ensuremath{-}overline{d}

CHIRAL QUARK MODEL ( QM) AND THE NUCLEON SPIN

asymmetry (E866) and the spin polarization functions, in the case of octet magnetic moments the results not only show improvement over the nonrelativistic quark model results but also give a nonzero value for the right hand side of the Coleman-Glashow sum rule, usually zero in most of the models. In the case of decuplet magnetic moments, we obtain a good overlap for

x-dependence of the quark distribution functions in the χCQMconfig

{ensuremath{Delta}}^{++},

Implications of η′ Coupling In The Chiral Constituent Quark Model

{ensuremath{Omega}}^{ensuremath{-}},