Abstract
A closed expression similar to the Ursell‐Mayer expansion is obtained for the static multiple density correlation function In=〈ρk1⋯ρkn of a many‐particle system. It is shown that In breaks into products of lower ones, if there exist partial momentum conservations among the k's. Using the convolution approximation for the n‐particle correlation function, we evaluate In in a closed form. The result is shown to be accurate in the small k region.