  We have considered here the statistics parameter for quasiparticles in FQH
states from an analysis of these states in the framework of chiral anomaly and
Berry phase. It is shown that we have a generalized relation such that the
statistical phase of a quasiparticle for FQH states at $\nu=p/q$ with $p(q)$
even or odd, is given by $e^{i\pi \theta}$ with $\theta=p/q $ and the charge is
$-e \frac{p}{q}$. The statistics parameter for a quasihole is identical with
that of a quasiparticle and the charge is of opposite sign.
