  The growth of superconducting order after an interaction quench in a
hexagonal lattice is studied. The cases of both time-reversal (TR) preserving
graphene, as well as the TR broken Haldane model are explored. Spin singlet
superconducting order is studied where the $s$, $d+id$, and $d-id$ wave orders
are the irreducible representations of the hexagonal lattice. For small
quenches, the $d$-wave order parameter grows the fastest, a result also
expected when the system is in thermal equilibrium. For the TR symmetry
preserving case, the growth rate of the two $d$-wave orders is identical, while
the TR-broken case prefers one of the chiral $d$-wave orders over the other,
leading to a TR broken topological superconductor. As the interaction quench
becomes larger, a smooth crossover is found where eventually the growth rate of
the $s$-wave becomes the largest. Thus for large interaction quenches, the
$s$-wave is preferred over the $d$-wave for both TR preserving and TR broken
systems. This result is explained in terms of the high energy quasi-particles
responsible for the dynamics as the interaction quench amplitude grows. The
results are relevant for time-resolved measurements that can probe the symmetry
of the superconducting fluctuations in a transient regime.
