  We explore the phase diagram of SU(2) Lattice Gauge Theory with dynamical
fermions in the temperature, mass, chemical potential space. We observe
qualitative changes of the dependence of the particle density on $\mu$ and $T$,
which is compatible with that expected of a gas of free massless quarks $n
\propto \mu^3$ only for $T \simeq T_c$. At the onset for thermodynamics the
interquark potential flattens at large separations, indicating enhanced fermion
screening and the transition to a deconfined phase. Temporal and spatial
Polyakov loops behave in different ways, the latter being nearly insensitive to
the chemical potential. The rotation of the chiral condensate to a baryonic
condensate, as inferred from the susceptibilities, might occur together with a
reduction of its magnitude in the chiral limit, possibly leading to a critical
temperature for diquark condensation smaller than the deconfinement
temperature. We further asses the r\^ole of the chemical potential into the
gauge dynamics by carrying out a partial quenched calculation. We speculate on
the relevance, or lack thereof, of our findings to real QCD.
