The concept of an injective affine embedding of the quantum states into a set
of classical states, i.e., into the set of the probability measures on some
measurable space, as well as its relation to statistically complete observables
is revisited, and its limitation in view of a classical reformulation of the
statistical scheme of quantum mechanics is discussed. In particular, on the
basis of a theorem concerning a non-denseness property of a set of coexistent
effects, it is shown that an injective classical embedding of the quantum
states cannot be supplemented by an at least approximate classical description
of the quantum mechanical effects. As an alternative approach, the concept of
quasi-probability representations of quantum mechanics is considered.Comment: 35 page