We argue that a new type of quantum Hall state requiring non-perturbative
Landau level mixing arises at low electron density. In these states, up and
down spin electrons pair to form spinless bosons that condense into a bosonic
quantum Hall state. We describe a wavefunction for a paired quantum Hall state
at ν=2 and argue that it is stabilized by a BCS instability arising in flux
attachment calculations. Based on this state, we derive a new global phase
diagram for the integral quantum Hall effect with spin. Additional experimental
implications are discussed.Comment: uufile, includes 4 page revtex file and 1 figure fil