We introduce a new field theory for studying quantum Hall systems. The
quantum field is a modified version of the bosonic operator introduce
d by Read. In contrast to Read's original work we do not work in the l
owest Landau level alone, and this leads to a much simpler formalism.
We identify an appropriate canonical conjugate field, and write a Hami
ltonian that governs the exact dynamics of our bosonic field operators
. We describe a Lagrangian formalism, derive the equations of motion f
or the fields and present a family of mean-field solutions. Finally, w
e show that these mean field solutions are precisely the Laughlin stat
es. We do not, in this work, address the treatment of fluctuations.