  Using the parent Lagrangian method together with a dimensional reduction from
$D$ to $(D-1)$ dimensions we construct dual theories for massive spin two
fields in arbitrary dimensions in terms of a mixed symmetry tensor
$T_{A[A_{1}A_{2}... A_{D-2}]}$. Our starting point is the well studied massless
parent action in dimension $D$. The resulting massive Stueckelberg-like parent
actions in $(D-1)$ dimensions inherits all the gauge symmetries of the original
massless action and can be gauge fixed in two alternative ways, yielding the
possibility of having either a parent action with a symmetric or a
non-symmetric Fierz-Pauli field $e_{AB}$. Even though the dual sector in terms
of the standard spin two field includes only the symmetrical part $e_{\{AB\}}$
in both cases, these two possibilities yield different results in terms of the
alternative dual field $T_{A[A_{1}A_{2}... A_{D-2}]}$. In particular, the
non-symmetric case reproduces the Freund-Curtright action as the dual to the
massive spin two field action in four dimensions.
