  One of the key signatures of the Quark Gluon Plasma (QGP) is the energy loss
of high momentum particles as they traverse the strongly interacting medium.
The energy loss of these particles is governed by the jet transport coefficient
$\hat{q}/T^3$, wherein it has been thought that there is a large jump as the
system transitions between the hadron gas and Quark Gluon Plasma phases. Here
we calculate $\hat{q}/T^3$ within the Hadron Resonance Gas (HRG) model with the
particle list PDG16+ and find that, if one incorporates the experimental error
in the hadronic calculation of $\hat{q}/T^3$ and assumes a higher
pseudo-critical temperature, then a smooth transition from the hadron gas phase
into the Quark Gluon Plasma phase is possible. We also find a significant
enhancement in $\hat{q}/T^3$ at finite baryon chemical potential and find
issues with the relationship between the shear viscosity and the jet transport
coefficient within a hadron gas phase.
