  Consistency of present-day lattice QCD simulations with dynamical (``sea'')
staggered fermions requires that the determinant of the staggered-fermion 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.
