Covariantly we reformulate the description of a spinning particle in t
erms of the Poincare group. We also construct a Lagrangian which entai
ls all possible constraints explicitly; all constraints can be obtaine
d just from the Lagrangian. Furthermore, in this covariant reformulati
on, the Lorentz element is to be considered to evolve the momentum or
spin component from an arbitrary fixed frame and not just from the par
ticle rest frame. Our system which is different from the usual formula
tion is directly comparable with the pseudoclassical formulation. We g
et a peculiar symmetry which resembles the supersymmetry of the pseudo
classical formulation.