Consistency of present-day lattice QCD simulations with dynamical ("sea") staggered fermions requires that the determinant of the staggeredfermion Dirac operator, det(D), be equal to det 4 (D rg ) det(T ) where D rg is a local one-flavor lattice Dirac operator, and T is a local operator containing only excitations with masses of the order of the cutoff. Using renormalization-group (RG) block transformations I show that, in the limit of infinitely many RG steps, the required decomposition exists for the free staggered operator in the "flavor representation." The resulting one-flavor Dirac operator D rg satisfies the Ginsparg-Wilson relation in the massless case. I discuss the generalization of this result to the interacting theory.