  Within the class of Derezi{\'n}ski-Enss pair-potentials which includes
Coulomb potentials a stationary scattering theory for $N$-body systems was
recently developed \cite {Sk1}. In particular the wave and scattering matrices
as well as the restricted wave operators are all defined at any non-threshold
energy, and this holds without imposing any a priori decay condition on channel
eigenstates. In this paper we improve for the case of $3$-body systems on the
known \emph{weak continuity} properties in that we show that all non-threshold
energies are \emph{stationary complete} in this case, resolving a conjecture
from \cite {Sk1} in the special case $N=3$. A consequence is that the above
scattering quantities depend \emph{strongly continuously} on the energy
parameter at all non-threshold energies, hence not only almost everywhere as
previously demonstrated (for an arbitrary $N$). Another consequence is that the
scattering matrix is unitary at any such energy. As a side result we give an
independent stationary proof of asymptotic completeness for $3$-body systems
with long-range pair-potentials. This is an alternative to the known
time-dependent proofs \cite{De, En}.
