  The density-of-states (DOS) for a magnetized (B) two-dimensional electron gas
(2DEG) containing point scatterers of arbitrary strengths, concentration
($n_s$) and distribution is analyzed. It is shown from the first principles
that for \(n_s \leq B/\Phi_o \equiv n_B\), the areal density of flux quanta
\(\Phi_o \equiv hc/e\), the DOS retains the extensive degeneracy characteristic
of the Landau levels, but reduced by a factor \((1 - {n_s}/{n_B})\). This
elementary but exact result gives a level condensation for magnetic field \(B >
n_s\Phi_o\), as first noted by Br\'{e}zin {\em et al.}. Its implications for
the Integral Quantum Hall Effect and for Random Matrix Theory are pointed out.
