We perform the complete bosonization of 2+1 dimensional QED with one f
ermionic flavor in the Hamiltonian formalism. The fermion operators ar
e explicitly constructed in terms of the vector potential and the elec
tric field. We carefully specify the regularization procedure involved
in the definition of these operators, and calculate the fermionic bil
inears and the energy-momentum tenser. The algebra of bilinears exhibi
ts the Schwinger terms which also appear in perturbation theory. The b
osonic Hamiltonian density is a local polynomial function of A(i) and
E(i), and we check explicitly the Lorentz invariance of the resulting
bosonic theory. Our construction is conceptually very similar to Mande
lstam's construction in 1+1 dimensions, and is dissimilar from the rec
ent bosonization attempts in 2+1 dimensions which hinge crucially on t
he existence of a Chern-Simons term.