Diquark and Baryon Masses in Composite Fermion Approach

A model for diquark has been suggested describing it as a Composite Fermion. The masses of the light[$\Lambda^{0}$, $\Sigma^{-}$, $\Xi^{-}$, $\Omega^{-}$], heavy [$\Lambda_{c}^{+}$, $\Sigma_{c}^{+}$, $\Xi_{c}^{0}$, $\Omega_{c}^{-}$ and $\Lambda_{b}^{0}$, $\Sigma_{b}^{0}$, $\Xi_{b}^{0}$, $\Omega_{b}^{-}$], doubly heavy [$\Xi_{cc}^{++}$, $\Xi_{cc}^{+}$, $\Xi_{cb}^{+}$, $\Xi_{cb}^{0}$, $\Xi_{bb}^{0}$, $\Xi_{bb}^{-}$, $\Omega_{cc}^{+}$, $\Omega_{cb}^{0}$, $\Omega_{bb}^{-}$] and triply heavy [$\Omega_{ccc}$, $\Omega_{ccb}$, $\Omega_{bbc}$, $\Omega_{bbb}$] baryons have been studied for J$^{P}$ = $\frac{1}{2}^{+}$ and $\frac{3}{2}^{+}$ states. The results are found to be in good agreement with available experimental data and other theoretical works