  Via molecular dynamics simulation with Langevin thermostat we study the
structure and dynamics of a flexible bead-spring active polymer model after a
quench from good to poor solvent conditions. The self propulsion is introduced
via a Vicsek-like alignment activity rule which works on each individual
monomer in addition to the standard attractive and repulsive interactions among
the monomeric beads. We observe that the final conformations are in the
globular phase for the passive as well as for all the active cases. By
calculating the bond length distribution, radial distribution function, etc.,
we show that the kinetics and also the microscopic details of these
\textit{pseudo equilibrium} globular conformations are not the same in all the
cases. Moreover, the center-of-mass of the polymer shows a more directed
trajectory during its motion and the behavior of the mean-squared-displacement
gradually changes from a super-diffusive to ballistic under the influence of
the active force in contrast to the diffusive behavior in the passive case.
