Abstract
An upper bound to the cross section for diffraction dissociation on a nucleus is derived by combining the fundamental viewpoint of Good and Walker with the eikonal model. The bound is consistent with measurements of πA(3π)A in the coherent region. A number of the observed features of diffractive production are shown to be understandable by assuming the existence of a complete set of states which are diagonal in nuclear matter, and which are absorbed approximately equally, as would be expected according to a naive quark model. A possible explanation for the apparent smallness of the absorption of 3π and 5π sytems in nuclei is given. Finally, speculations are made on how these results might apply to diffractive production on proton targets.