We show that the use of the fourth-root trick in lattice QCD with staggered
fermions corresponds to a non-local theory at non-zero lattice spacing, but
argue that the non-local behavior is likely to go away in the continuum limit.
We give examples of this non-local behavior in the free theory, and for the
case of a fixed topologically non-trivial background gauge field. In both
special cases, the non-local behavior indeed disappears in the continuum limit.
Our results invalidate a recent claim that at non-zero lattice spacing an
additive mass renormalization is needed because of taste-symmetry breaking.Comment: 17 pages, two refs. and a note adde