  We present predictions for jet suppression from small to intermediate to very
large radius, for low and very high energy jets created in heavy ion collisions
at the LHC. We use the hybrid strong/weak coupling model for jet quenching that
combines perturbative shower evolution with an effective strongly coupled
description of the energy and momentum transfer from the jet into the
hydrodynamic quark-gluon plasma. Because of momentum conservation, the wake
created by the jet enhances or depletes the amount of particles generated at
the freeze-out hypersurface depending on their orientation with respect to the
jet. Within such framework we find that jet suppression is surprisingly
independent of the anti-$k_T$ radius $R$, first slightly increasing as one
increases $R$, then at larger values of $R$ very slowly decreasing. This nearly
independence of jet suppression with increasing values of $R$ arises from two
competing effects, namely the larger energy loss of the hard jet components,
which tends to increase suppression, versus the partial recovery of the lost
energy due to medium response, reducing suppression. We also find that the
boosted medium from the recoiling jet reduces the amount of plasma in the
direction opposite to it in the transverse plane, increasing the amount of jet
suppression due to an over-subtraction effect. We show that this characteristic
signature of the hydrodynamization of part of the jet energy can be quantified
by selecting samples of dijet configurations with different relative
pseudorapidities between the leading and the subleading jet.
