Strongly correlated two dimensional electrons are believed to form a spin
liquid in some regimes of density and temperature. As the density is varied,
one expects a transition from this spin liquid state to a spin density wave
antiferromagnetic state. In this paper we show that it is self-consistent to
assume that this transition is second order and, on this assumption, determine
the critical behavior of the 2pF susceptibility, the NMR rates T1 and
T2 and the uniform susceptibility. We compare our results to data on high
Tc materials.Comment: 14 pages, 6 Postscript figures in a separate fil