They mean that the condition that the $2n$-form be nonzero gives an open condition on the vector space of closed complex $1$-forms. This follows immediately because the function $f\colon \mathcal A^1(M)\to\mathcal A^{2n}(M)\cong \mathcal A^0(M)$ given by $f(\Omega) = \omega^{n-1}\wedge\Omega\wedge\bar\Omega$ is continuous. (By $\mathcal A^k(M)$ I mean the space of complex-valued $k$-forms on $M$. Because $M$ is compact, it's easy to put norms on these vector spaces, if you so desire.) Intuitively, this means that if we wiggle $\Omega$ slightly, the wedge product varies only slightly and hence stays nonzero.