We have considered the fractional quantum Hall effect from the view po
int of the deformation of the symplectic structure on phase space. We
have shown that on the phase space each quantized Hall particle in a n
u = 1/m FQHE state occupies an area Delta p Delta q = 2 pi m (h) over
bar, m being an odd integer, where m originates from the inherent geom
etry of our formalism. (C) 1998 Published by Elsevier Science B.V.