We consider a family of cylindrical spacetimes endowed with angular momentu
m that are solutions to the vacuum Einstein equations outside the symmetry
axis. This family was recently obtained by performing a complete gauge fixi
ng adapted to cylindrical symmetry. In this paper, we find boundary conditi
ons that ensure that the metric arising from this gauge fixing is well defi
ned and that the resulting reduced system has a consistent Hamiltonian dyna
mics. These boundary conditions must be imposed both on the symmetry axis a
nd in the region far from the axis at spacelike infinity. Employing such co
nditions, we determine the asymptotic behaviour of the metric close to and
far from the axis. In each of these regions, the approximate metric describ
es a conical geometry with a time dislocation. In particular, around the sy
mmetry axis the effect of the singularity consists in inducing a constant d
eficit angle and a timelike helical structure. Based on these results and o
n the fact that the degrees of freedom in our family of metrics coincide wi
th those of cylindrical vacuum gravity, we argue that the analysed set of s
pacetimes represent cylindrical gravitational waves surrounding a spinning
cosmic string. For any of these spacetimes, a prediction of our analysis is
that the wave content increases the deficit angle at spatial infinity with
respect to that detected around the axis.