Recently, Cohen has proposed a construction for joint distributions of
arbitrary physical quantities, in direct generalization of joint time
-frequency representations. Actually, this method encompasses two appr
oaches: one based on operator correspondences and one based on weighti
ng kernels. The literature has emphasized the kernel method due to its
ease of analysis; however, its simplicity comes at a price. In this l
etter, we use a simple example to demonstrate that the kernel method c
annot generate all possible bilinear joint distributions. Our results
suggest that the relationship between the operator method and the kern
el method merits closer scrutiny.