  Baryon-strangeness correlations ($C_{BS}$) are studied with a hadron/string
transport approach (UrQMD) and a dynamical quark recombination model (quark
molecular dynamics, qMD) for various energies from $E_{lab}=4A$ GeV to
$\sqrt{s_{NN}}=200$ GeV. As expected, we find that the hadron/string dynamics
shows correlations similar to a simple hadron gas. In case of the quark
molecular dynamics, we find that initially the $C_{BS}$ correlation is that of
a weakly interacting QGP but changes in the process of hadronization also to
the value for a hadron gas. Therefore, we conclude that the hadronization
process itself makes the initial baryon strangeness correlation unobservable.
To make an experimental study of this observable more feasible, we also
investigate how a restriction to only charged kaons and $\Lambda$'s (instead of
all baryons and all strange particles) influences the theoretical result on
$C_{BS}$. We find that a good approximation of the full result can be obtained
in this limit in the present simulation.
